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Sample records for 3p cu 3s

  1. Intercombination decay of 3s3p3P10 in Mg I-like Ni and Cu

    The intercombination transition 3s21S0-3s3p 3p10 in Ni16+ and Cu17+ has been studied by beam-foil spectroscopic methods. Decay curve analysis yields lifetime values of (12.0+-1.0) ns and (8.8+-0.6) ns for Ni and Cu in agreement with various predictions. (orig./WL)

  2. A study of angle-resolved photoemission extended fine structure as applied to the Ni 3p, Cu 3s, and Cu 3p core levels of the respective clean (111) surfaces

    Huff, W.R.A.; Moler, E.J.; Kellar, S.A. [Lawrence Berkeley National Lab., CA (United States)] [and others

    1997-04-01

    The first non-s initial state angle-resolved photoemission extended fine structure (ARPEFS) study of clean surfaces for the purpose of further understanding the technique is reported. The surface structure sensitivity of ARPEFS applied to clean surfaces and to arbitrary initial states is studied using normal photoemission data taken from the Ni 3p core levels of a Ni(111) single crystal and the Cu 3s and the Cu 3p core-levels of a Cu(111) single crystal. The Fourier transforms of these clean surface data are dominated by backscattering. Unlike the s initial state data, the p initial state data show a peak in the Fourier transform corresponding to in-plane scattering from the six nearest-neighbors to the emitter. Evidence was seen for single-scattering events from in the same plane as the emitters and double-scattering events. Using a newly developed, multiple-scattering calculation program, ARPEFS data from clean surfaces and from p initial states can be modeled to high precision. Although there are many layers of emitters when measuring photoemission from a clean surface, test calculations show that the ARPEFS signal is dominated by photoemission from atoms in the first two crystal layers. Thus, ARPEFS applied to clean surfaces is sensitive to surface reconstruction. The known contraction of the first two Cu(111) layers is confirmed. The best-fit calculation for clean Ni(111) indicates an expansion of the first two layers. To better understand the ARPEFS technique, the authors studied s and non-s initial state photoemission from clean metal surfaces.

  3. A study of angle-resolved photoemission extended fine structure as applied to the Ni 3p, Cu 3s, and Cu 3p core levels of the respective clean (111) surfaces

    The first non-s initial state angle-resolved photoemission extended fine structure (ARPEFS) study of clean surfaces for the purpose of further understanding the technique is reported. The surface structure sensitivity of ARPEFS applied to clean surfaces and to arbitrary initial states is studied using normal photoemission data taken from the Ni 3p core levels of a Ni(111) single crystal and the Cu 3s and the Cu 3p core-levels of a Cu(111) single crystal. The Fourier transforms of these clean surface data are dominated by backscattering. Unlike the s initial state data, the p initial state data show a peak in the Fourier transform corresponding to in-plane scattering from the six nearest-neighbors to the emitter. Evidence was seen for single-scattering events from in the same plane as the emitters and double-scattering events. Using a newly developed, multiple-scattering calculation program, ARPEFS data from clean surfaces and from p initial states can be modeled to high precision. Although there are many layers of emitters when measuring photoemission from a clean surface, test calculations show that the ARPEFS signal is dominated by photoemission from atoms in the first two crystal layers. Thus, ARPEFS applied to clean surfaces is sensitive to surface reconstruction. The known contraction of the first two Cu(111) layers is confirmed. The best-fit calculation for clean Ni(111) indicates an expansion of the first two layers. To better understand the ARPEFS technique, the authors studied s and non-s initial state photoemission from clean metal surfaces

  4. Relativistic calculations of 3s21S0-3s3p 1P1 and 3s21S0-3s3p 3P1,2 transition probabilities in the Mg isoelectronic sequence

    Using the multi-configuration Dirac—Fock self-consistent field method and the relativistic configuration-interaction method, calculations of transition energies, oscillator strengths and rates are performed for the 3s21S0-3s3p 1P1 spin-allowed transition, 3s21S0-3s3p 3P1,2 intercombination and magnetic quadrupole transition in the Mg isoelectronic sequence (Mg I, Al II, Si III, P IV and S V). Electron correlations are treated adequately, including intravalence electron correlations. The influence of the Breit interaction on oscillator strengths and transition energies are investigated. Quantum electrodynamics corrections are added as corrections. The calculation results are found to be in good agreement with the experimental data and other theoretical calculations. (atomic and molecular physics)

  5. Size-tunable, hexagonal plate-like Cu3P and Janus-like Cu-Cu3P nanocrystals.

    De Trizio, Luca; Figuerola, Albert; Manna, Liberato; Genovese, Alessandro; George, Chandramohan; Brescia, Rosaria; Saghi, Zineb; Simonutti, Roberto; Van Huis, Marijn; Falqui, Andrea

    2012-01-24

    We describe two synthesis approaches to colloidal Cu(3)P nanocrystals using trioctylphosphine (TOP) as phosphorus precursor. One approach is based on the homogeneous nucleation of small Cu(3)P nanocrystals with hexagonal plate-like morphology and with sizes that can be tuned from 5 to 50 nm depending on the reaction time. In the other approach, metallic Cu nanocrystals are nucleated first and then they are progressively phosphorized to Cu(3)P. In this case, intermediate Janus-like dimeric nanoparticles can be isolated, which are made of two domains of different materials, Cu and Cu(3)P, sharing a flat epitaxial interface. The Janus-like nanoparticles can be transformed back to single-crystalline copper particles if they are annealed at high temperature under high vacuum conditions, which makes them an interesting source of phosphorus. The features of the Cu-Cu(3)P Janus-like nanoparticles are compared with those of the striped microstructure discovered more than two decades ago in the rapidly quenched Cu-Cu(3)P eutectic of the Cu-P alloy, suggesting that other alloy/eutectic systems that display similar behavior might give origin to nanostructures with flat, epitaxial interface between domains of two diverse materials. Finally, the electrochemical properties of the copper phosphide plates are studied, and they are found to be capable of undergoing lithiation/delithiation through a displacement reaction, while the Janus-like Cu-Cu(3)P particles do not display an electrochemical behavior that would make them suitable for applications in batteries. PMID:22136519

  6. KⅧ-TbLⅣ离子3s3p 3P1-3s2 1S0 的自旋禁戒跃迁%Intercombination Transitions 3s3p 3P1-3s2 1S0 in Magnesium-like Ions through KⅧ to TbLⅣ

    牟致栋; 魏琦瑛

    2004-01-01

    在对KⅧ-TbLⅣ离子3s3p 3P1能级结构的多组态相互作用理论HXR方法计算的基础上, 分析了各种效应对等电子序列离子能级结构的影响, 找出了能级沿等电子序列变化的规律性. 预测计算了K Ⅷ-Tb LⅣ离子3s3p 3P1的能级. 由此进一步计算了KⅧ-TbL Ⅳ离子自旋禁戒跃迁3s3p 3P1-3s2 1S0的谱线波长、振子强度和跃迁概率.

  7. Synthesization of the Ar VIII 3s-3p beam-foil decay curve

    The beam-foil decay curve for the 3s-3p transition in Ar VIII has been simulated from experimentally determined relative initial level populations and transition probabilities calculated in the numerical Coulomb approximation. Good agreement is observed between simulated and measured decay curves. A discussion of the simulation is given. (Auth.)

  8. Transition probabilities for the 3s2 3p(2P0)-3s3p2(4P) intersystem lines of Si II

    Calamai, Anthony G.; Smith, Peter L.; Bergeson, S. D.

    1993-01-01

    Intensity ratios of lines of the spin-changing 'intersystem' multiplet of S II (4P yields 2P0) at 234 nm have been used to determine electron densities and temperatures in a variety of astrophysical environments. However, the accuracy of these diagnostic calculations have been limited by uncertainties associated with the available atomic data. We report the first laboratory measurement, using an ion-trapping technique, of the radiative lifetimes of the three metastable levels of the 3s3p2 4P term of Si II. Our results are 104 +/- 16, 406 +/- 33, and 811 +/- 77 micro-s for lifetimes of the J = 1/2, 5/2, and 3/2 levels, respectively. A-values were derived from our lifetimes by use of measured branching fractions. Our A-values, which differ from calculated values by 30 percent or more, should give better agreement between modeled and observed Si II line ratios.

  9. Au Nanowire-Striped Cu3P Platelet Photoelectrocatalysts.

    Dutta, Anirban; Samantara, Aneeya K; Adhikari, Samrat Das; Jena, Bikash Kumar; Pradhan, Narayan

    2016-03-17

    A stripy pattern of continuous epitaxial growth of thin Au nanowires on plasmonic Cu3P platelets is reported. The obtained Au-Cu3P heterostructures retain their wide area interfacial heterojunction, which is typically not observed in metal-semiconductor heterostructures. This is performed by phosphine-mediated in situ reduction of Au ions on specific facets of Cu3P platelets. The intriguing stripy movements of nanowires are regulated by strong surface binding ligands. Because this is a dual plasmon heterostructure with wide visible absorption window, these are further explored as a photoelectrocatalyst for efficient hole transfer and sensing of an important biomolecule, nicotinamide adenine dinucleotide (NADH). The observed anodic photocurrent was 30 times higher in the presence of NADH, and this proves that the heterostructured material is an ideal photosenser and an efficient catalyst for solar energy conversion. PMID:26938025

  10. Relativistic calculations of 3s2 1S0-3s3p 1P1 and 3s2 1S0-3s3p 3P1,2 transition probabilities in the Mg isoelectronic sequence

    Cheng Cheng; Gao Xiang; Qing Bo; Zhang Xiao-Le; Li Jia-Ming

    2011-01-01

    Using the multi-configuration Dirac-Fock self-consistent field method and the relativistic configuration-interaction method, calculations of transition energies, oscillator strengths and rates are performed for the 3s2 1S0-3s3p 1P1 spinallowed transition, 3s2 1S0-3s3p 3P1,2 intercombination and magnetic quadrupole transition in the Mg isoelectronic sequence (Mg Ⅰ, Al Ⅱ, Si ⅢⅢ, P Ⅳ and S Ⅴ). Electron correlations are treated adequately, including intravalence electron correlations. The influence of the Breit interaction on oscillator strengths and transition energies are investigated. Quantum electrodynamics corrections are added as corrections. The calculation results are found to be in good agreement with the experimental data and other theoretical calculations.

  11. Radiative rates for E1, E2, M1, and M2 transitions among the 3s$^2$3p$^5$, 3s3p$^6$, and 3s$^2$3p$^4$3d configurations of Cl-like W LVIII

    Aggarwal, K M

    2014-01-01

    We report calculations of energy levels, radiative decay rates, and lifetimes for transitions among the 3s$^2$3p$^5$, 3s3p$^6$, and 3s$^2$3p$^4$3d configurations of Cl-like W LVIII. The general-purpose relativistic atomic structure package (GRASP) has been adopted for our calculations. Comparisons are made with the most recent results of Mohan et al. [Can. J. Phys. {\\bf 92} (2014) xxx] and discrepancies in lifetimes are noted, up to four orders of magnitude in some instances. Our energy levels are estimated to be accurate to better than 0.5\\%, whereas results for radiative rates and lifetimes should be accurate to better than 20\\%.

  12. 类硅铑离子的3s23p23P1,2-3s3p35S2的跃迁谱线%The Intercombination Lines of 3s23p23P1,2-3s3p35S2 in Si-like Ions, Rhodium

    2002-01-01

    用束箔法研究了类硅铑离子的3s23p23P1,2-3s3p35S2的禁戒跃迁谱线.谱线识别从已知基态精细结构的分裂、基于分支比的强度比、相似的衰减特性、离子束能量下的谱线预期值方面着手.识别后,通过对已知谱线的波长的等电子系列曲线插值或外推来获得用于较刻的谱线的波长,然后较刻出3s23p23P1,2-3s3p35S2这两条谱线.

  13. Electron Excitation Cross Sections for the S II Transitions: 3s(exp 2)3p(exp 3) 4S(exp o) approaches 3s(exp 2)3p(exp 3) 2D(exp o), 2P(exp o), and 3s3p(exp 4) 4P

    Liao, C.; Chutjian, A.; Hitz, D.; Tayal, S. S.

    1997-01-01

    Experimental and theoretical collisional excitation cross sections are reported for the transitions 3s(exp 2)3p(exp 3)4S(exp o) approaches 3s(exp 2)3p(exp 3) 2D(exp o), 2P(exp o), and 3s3P(exp 4) 4P in S II. The transition wavelengths (energies) are 6716 A (1.85 eV), 4069 A (3.05 eV), and 1256 A (9.87 eV), respectively. In the experiments, use is made of the energy-loss merged-beams method. The metastable fraction of the S II beam was assessed and minimized. The contribution of elastically scattered electrons was reduced by the use of a lowered solenoidal magnetic field and a modulated radio-frequency voltage on the analyzing plates and by retarding grids to reject the elastically scattered electrons with larger Larmor radii. For each transition, comparisons are made among experiments, the new 19 state R-matrix calculation, and three other close-coupling calculations.

  14. The Cu2FeTi3S8 and Cu2FeZr3S8 compounds: Crystal structure and electroanalytical application

    The Cu2FeTi3S8 and Cu2FeZr3S8 compounds were produced by solid-state synthesis. The crystal structure of the quaternary phases was investigated by X-ray powder method. The compounds are described in the thiospinel structure (space group Fd3-bar m) with the unit cell parameters a = 1.00099(1) nm (Cu2FeTi3S8) and a = 1.03837(2) nm (Cu2FeZr3S8). The atomic parameters were calculated in the isotropic approximation (RI = 0.0496 and RI = 0.0422 for Cu2FeTi3S8 and Cu2FeZr3S8, respectively). Iron(III)-selective electrodes were prepared using the chalcogenide compounds Cu2FeTi3S8 and Cu2FeZr3S8. The electrode function slopes are 52.7 mV/pC for Cu2FeTi3S8 and 66.2 mV/pC for Cu2FeZr3S8, the detection limits are 1 x 10-5 M and 2 x 10-5 M respectively. The prepared electrochemical sensors are not sensitive to Cd2+, Zn2+, Mn2+, Ni2+, Co2+, Mg2+, Cr3+, and Fe2+ ions, and were tested in the potentiometric titration of Fe(III) with EDTA solution.

  15. Experimental Determination of the 24Mg I (3s3p)3P2 Lifetime

    Jensen, Brian Bak; He, Ming; Westergaard, Philip Grabow;

    2011-01-01

    We present the first experimental determination of the electric-dipole forbidden (3s3p)3P2¿(3s2)1S0 (M2) transition rate in 24Mg and compare to state-of-the-art theoretical predictions. Our measurement exploits a magnetic trap isolating the sample from perturbations and a magneto-optical trap as an...

  16. Stark broadening of 3s 3P0-3p 3D and 3p 3D-3d 3F0 transitions along carbon isoelectronic sequences of ions revisited

    The Stark widths of N II and O III spectral lines belonging to 3s 3P0-3p 3D and 3p 3D-3d 3F0 multiplets have been calculated and measured in a capillary discharge plasma. The calculations are extended to the same multiplets of F IV and Ne V ions. The plasma electron density in the capillary discharge is determined from the width of the He II Pβ line, while the electron temperature is measured from the relative intensities of N II lines. A comparison of the experimental and theoretical data shows good mutual agreement, which is well within the estimated experimental and theoretical uncertainties. The theory predicts the ratio of the corresponding N II to O III line widths to be larger than unity, in disagreement with our earlier experiment in a pulsed arc. In the new experiment, where all spectral lines were recorded under the same plasma conditions, the theoretical predictions and the results of the capillary experiment are in agreement. The possible sources of an error in the earlier experiment are indicated

  17. Cu6Te3S. A Cu-filled Cr3Si-structure variant

    A solid state melting and annealing route was used to prepare Cu6Te3S, a copper telluride sulfide representing a filled variant of the Cr3Si structure type. The title compound exhibits a reversible phase transition at 404 K which was confirmed by thermal analysis, temperature dependent X-ray single crystal and powder diffractometry. Both polymorphs crystallize cubic in space groups P anti 43n and P213, respectively. X-ray photoelectron spectroscopy (XPS) was performed to evaluate the electronic structure of Cu6Te3S and to determine the oxidation state of Cu in the title compound.

  18. Influence of Optical Properties on the Spin Polarization of Cu3P Photoelectrons

    Chassé, A.; Niebergall, L.

    We have investigated the influence of optical properties of Cu(001) on the spin polarization in Cu3p photoelectron diffraction patterns. The refraction and absorption of light have been taken into account in the calculation of the dipole transition matrix element. Therefore, a general polarization vector of light is defined within a macroscopic theory of electromagnetic fields. Results are shown and discussed for Cu3p photoelectrons excited by linearly or circularly polarized light, respectively. It is shown that the optical behavior of crystals may cause a symmetry breaking in the angular dependence of the photoelectron intensity. Besides, there are strong quantitative changes in the related spin polarization of Cu3p photoelectrons.

  19. 'Oxygen' effect in ionization loss spectrum of Cu3p in YBa2Cu3Ox ceramics

    YBaCu3Ox ceramic samples with different oxygen concentration (6.2; 6.5 and 6.9) in a volume are investigated. The process of degradation of samples with high X in the vacuum is analyzed. The surface purification is performed through scribing in argon atmosphere. A new effect is ascertained which is manifested in high sensitivity of Cu3p ionization loss spectrum to the density of the non-occupied electron states at the Fermi level. It is shown that Cu3p ionization spectrum can serve as a new criterion of superconductor surface quality from the viewpoint of its electronic structure

  20. Redox mechanism in the binary transition metal phosphide Cu3P

    Mauvernay, B.; Doublet, M.-L.; Monconduit, L.

    2006-05-01

    The electrochemical behaviour of the binary transition metal phosphide Cu3P towards lithium is investigated through galvano- and potentiostatic measurements. Obtained through high-temperature synthesis, this system shows a better volumetric capacity than graphite and a good capacity retention. In situ X-ray diffraction and first-principles electronic structure calculations are combined with the electrochemical results to show that the complete insertion of 3Li+ in the Cu3P electrode proceeds with the formation of three intermediate phases of lithium composition LixCu(3-x)P (x=1,2,3). The extra capacity previously observed in discharge is now clearly assigned to lithium insertion into the CuP2 impurity and to SEI reactions.

  1. Long-range interactions between a He($2 ^3S$) atom and a He($2 ^3P$) atom for like isotopes

    Zhang, J Y; Sadeghpour, H R; Vrinceanu, D; Yan, Z C; 10.1103/.73.022710

    2006-01-01

    For the interactions between a He($2 ^3S$) atom and a He($2 ^3P$) atom for like isotopes, we report calculations of the coefficients determining the potential energies at large internuclear separations. Using accurate variational wave functions in Hylleraas coordinates we evaluate the coefficient $C_{3}$ of the resonant dipole-dipole energy, and the van der Waals coefficients $C_{6}$, $C_{8}$, and $C_{10}$ of the energies arising from the mutual perturbations of instantaneous electric dipole, quadrupole, and octupole interactions. We establish definitive values including treatment of the finite nuclear mass for the ${}^3$He($2 ^3S$)--${}^3$He($2 ^3P$) and ${}^4$He($2 ^3S$)--${}^4$He($2 ^3P$) interactions.

  2. Theoretical study of Na(4p2P)+Na(3s2S) and Cd(5p3P0)+Na(3s2S) collisions and their role in the energy transfer between Cd* and Na

    We have computed the cross sections for the energy transfer process Cd(5p3P0) + Na(3s2S) →Cd(5s1S) + Na(4p2P) and for the state changing collision Na(4p2P) + Na(3s2S)→Na(3d2D) + Na(3s2S), based on theoretical interaction potentials for the NaCd and Na2 systems, respectively. Our calculations shed light on the interpretation of experiments with laser excited Na+Cd vapour mixtures. It turns out that Cd(5p3P0), in rapid equilibrium with the doorway state Cd(5p3P1), efficiently transfers energy to Na, populating the 4p2P state. The collisions with ground state Na cause a very fast conversion of the 4p2P to the 3d2D state, from which the strongest emission is observed. (orig.)

  3. Isotope shifts of the (3s3p) 3P0,1,2-(3s4s) 3S1 Mg I transitions

    He, Ming; Therkildsen, Kasper T.; Jensen, Brian B.;

    2009-01-01

    We report measurements of the isotope shifts of the (3s3p)P30,1,2-(3s4s)S31 Mg I transitions for the stable isotopes M24g (I=0) , M25g (I=5/2) , and M26g (I=0) . Furthermore, the M25g S31 hyperfine coefficient A(S31)=(-321.6±1.5)MHz is extracted and found to be in excellent agreement with state...

  4. Reverse energy-pooling collisions: K(5D)+Na(3S)→K(4P)+Na(3P)

    The observation of a heteronuclear reverse energy pooling process is reported. The cross section for the collision processes K(5D)+Na(3S)→K(4P)+Na(3P) has been measured and compared to calculations carried out using a multicrossing Landau-Zener model. copyright 1997 The American Physical Society

  5. Effects on intercombination transition rates and branching ratios-the UV0.01 (3s{sup 2}3p{sup 2} {sup 3}P{sub 1,2} - 3s3p{sup 3} {sup 5}S{sub 2}) multiplet in Si I-like ions revisited

    Andersson, Martin; Brage, Tomas [Department of Physics, Lund University, Box 118, SE-221 00 Lund (Sweden)

    2007-02-28

    We report on large-scale ab initio calculations for intercombination lines in Si I-like ions. Two measurable quantities, the lifetime of the 3s3p{sup 3} {sup 5}S{sub 2} level and the branching ratio of the two lines are discussed, to infer the importance of different features of our calculations. The effects of core polarization, two-body spin-dependent operators and Dirac contra Breit-Pauli approaches are discussed. Earlier calculations are reviewed and evaluated. The calculated lifetimes are in good agreement with experiments, while a discrepancy persists for branching ratios.

  6. Auger Spectra and Different Ionic Charges Following 3s, 3p and 3d Sub-Shells Photoionization of Kr Atoms

    Yehia A. Lotfy

    2006-01-01

    Full Text Available The decay of inner-shell vacancy in an atom through radiative and non-radiative transitions leads to final charged ions. The de-excitation decay of 3s, 3p and 3d vacancies in Kr atoms are calculated using Monte-Carlo simulation method. The vacancy cascade pathway resulted from the de-excitation decay of deep core hole in 3s subshell in Kr atoms is discussed. The generation of spectator vacancies during the vacancy cascade development gives rise to Auger satellite spectra. The last transitions of the de-excitation decay of 3s, 3p and 3d holes lead to specific charged ions. Dirac-Fock-Slater wave functions are adapted to calculate radiative and non-radiative transition probabilities. The intensity of Kr^{4+} ions are high for 3s hole state, whereas Kr^{3+} and Kr^{2+} ions have highest intensities for 3p and 3d hole states, respectively. The present results of ion charge state distributions agree well with the experimental data.

  7. Calculation of the photo-electrons angular distribution asymmetry parameter β2p near the (3s3p)Ip resonance of He

    Near the (3s3p)1p resonance of He, we have calculated the photo-electrons angular distribution asymmetry parameter β2p in the diagonalization approximation. Using the measured value of βn=2 near the (3s3p)1p level obtained by Lindle et al. in the resonance photo-ionization of He to He+(n=2), we have estimated the ratio R=σ2p/σ2s of the partial 2p photo-ionization cross section to the partial 2s photo-ionization cross section. Our calculation supports the result that in the resonance region, the formation of ions in the 2p level dominates over the 2s level. This is in good agreement with the experimental and most of the theoretical results reported to date. (author). 18 refs, 1 fig., 2 tabs

  8. High current Cu3P liquid metal ion source using a novel extractor configuration

    Higuchi-Rusli, R. H.; Corelli, J. C.

    1987-12-01

    It has been found that by utilizing a sharp needle for the extractor electrode in close proximity to the source tip wetted with Cu3P liquid alloy, a large increase (factor ˜300) in ion current is observed in comparison to standard liquid metal ion sources (LMIS's). In standard previously used LMIS's the extractor electrode was a flat plane with a circular hole centered on the source needle tip. This new high current source has important applications in focused and broad ion beam deposition systems.

  9. Colloidal CdSe/Cu3P/CdSe nanocrystal heterostructures and their evolution upon thermal annealing.

    De Trizio, Luca; De Donato, Francesco; Casu, Alberto; Genovese, Alessandro; Falqui, Andrea; Povia, Mauro; Manna, Liberato

    2013-05-28

    We report the synthesis of colloidal CdSe/Cu(3)P/CdSe nanocrystal heterostructures grown from hexagonal Cu(3)P platelets as templates. One type of heterostructure was a sort of "coral", formed by vertical pillars of CdSe grown preferentially on both basal facets of a Cu(3)P platelet and at its edges. Another type of heterostructure had a "sandwich" type of architecture, formed by two thick, epitaxial CdSe layers encasing the original Cu(3)P platelet. When the sandwiches were annealed under vacuum up to 450 °C, sublimation of P and Cd species with concomitant interdiffusion of Cu and Se species was observed by in situ HR- and EFTEM analyses. These processes transformed the starting sandwiches into Cu2Se nanoplatelets. Under the same conditions, both the pristine (uncoated) Cu(3)P platelets and a control sample made of isolated CdSe nanocrystals were stable. Therefore, the thermal instability of the sandwiches under vacuum might be explained by the diffusion of Cu species from Cu(3)P cores into CdSe domains, which triggered sublimation of Cd, as well as out-diffusion of P species and their partial sublimation, together with the overall transformation of the sandwiches into Cu(2)Se nanocrystals. A similar fate was followed by the coral-like structures. These CdSe/Cu(3)P/CdSe nanocrystals are therefore an example of a nanostructure that is thermally unstable, despite its separate components showing to be stable under the same conditions. PMID:23557168

  10. Cross sections for the excitation of 3s,3p,3d,4p, and 4s manifolds in e-Ne collisions

    Theoretical differential and integral cross sections are reported for inelastic scattering of electrons by neon atoms for incident electron energies in the range of 20-100 eV. Transitions from the ground state to forty states associated with the 3s, 3p, 3d, 4s, and 4p manifolds were considered. The methods employed were the distorted wave approximation and first-order many-body theory, where the distorting potential includes the static-exchange potential. A comparison of our results with experimental data and other theoretical results are shown and discussed. (author)

  11. Radiative lifetime of the 3s3p exp 3(exp 5 S sub 2 exp 0) metastable level of P(+)

    Calamai, Anthony G.; Han, Xiaofeng; Parkinson, William H.

    1992-01-01

    The present experimental and theoretical results for the radiative lifetime of the 3s3p exp 3(exp 5 S sub 2 exp 0) metastable level of P(+) encompass an experimental determination of the (exp 5 S sub 2 exp 0) lifetime which represents the first measured lifetime of a low charge-state ion in the Si I sequence. This constitutes a fundamental test of the theoretical methods used to determine transition possibilities for intercombination lines involving this level, and suggests that theoretical techniques used to determine such transition probabilities in low-Z species of the Si I isoelectronic sequence should be reevaluated.

  12. Characterization of Cu3P phase in Sn3.0Ag0.5Cu0.5P/Cu solder joints

    Jian-xun Chen; Xing-ke Zhao; Xu-chen Zou; Ji-hua Huang; Hai-chun Hu; Hai-lian Luo

    2014-01-01

    This article reports the effects of phosphorus addition on the melting behavior, microstructure, and mechanical properties of Sn3.0Ag0.5Cu solder. The melting behavior of the solder alloys was determined by differential scanning calorimetry. The interfacial micro-structure and phase composition of solder/Cu joints were studied by scanning electron microscopy and energy dispersive spectrometry. Thermodynamics of Cu-P phase formation at the interface between Sn3.0Ag0.5Cu0.5P solder and the Cu substrate was characterized. The results indicate that P addition into Sn3.0Ag0.5Cu solder can change the microstructure and cause the appearance of rod-like Cu3P phase which is distributed randomly in the solder bulk. The Sn3.0Ag0.5Cu0.5P joint shows a mixture of ductile and brittle fracture after shear test-ing. Meanwhile, the solidus temperature of Sn3.0Ag0.5Cu solder is slightly enhanced with P addition.

  13. Characterization of Cu3P phase in Sn3.0Ag0.5Cu0.5P/Cu solder joints

    Chen, Jian-xun; Zhao, Xing-ke; Zou, Xu-chen; Huang, Ji-hua; Hu, Hai-chun; Luo, Hai-lian

    2014-01-01

    This article reports the effects of phosphorus addition on the melting behavior, microstructure, and mechanical properties of Sn3.0Ag0.5Cu solder. The melting behavior of the solder alloys was determined by differential scanning calorimetry. The interfacial microstructure and phase composition of solder/Cu joints were studied by scanning electron microscopy and energy dispersive spectrometry. Thermodynamics of Cu-P phase formation at the interface between Sn3.0Ag0.5Cu0.5P solder and the Cu substrate was characterized. The results indicate that P addition into Sn3.0Ag0.5Cu solder can change the microstructure and cause the appearance of rod-like Cu3P phase which is distributed randomly in the solder bulk. The Sn3.0Ag0.5Cu0.5P joint shows a mixture of ductile and brittle fracture after shear testing. Meanwhile, the solidus temperature of Sn3.0Ag0.5Cu solder is slightly enhanced with P addition.

  14. Effects on intercombination transition rates and branching ratios-the UV0.01 (3s23p23P1,2 - 3s3p35S2) multiplet in Si I-like ions revisited

    We report on large-scale ab initio calculations for intercombination lines in Si I-like ions. Two measurable quantities, the lifetime of the 3s3p35S2 level and the branching ratio of the two lines are discussed, to infer the importance of different features of our calculations. The effects of core polarization, two-body spin-dependent operators and Dirac contra Breit-Pauli approaches are discussed. Earlier calculations are reviewed and evaluated. The calculated lifetimes are in good agreement with experiments, while a discrepancy persists for branching ratios

  15. Measurement of the spin-forbidden decay rate (3s3d)1D2¿(3s3p)3 P2,1 in 24Mg

    Therkildsen, K. T.; Jensen, Brian Bak; Ryder, C. P.; Malossi, N.; Thomsen, Jan Westenkær

    2009-01-01

    We have measured the spin-forbidden decay rate from (3s3d)D12¿(3s3p)P32,1 in M24g atoms trapped in a magneto-optical trap. The total decay rate, summing up both exit channels (3s3p)P31 and (3s3p)P32 , yields 196±10s-1 in excellent agreement with resent relativistic many-body calculations of Porsev...

  16. Excitation of the OI (3s 5S0-3p 5P; lambda 7774 A) multiplet by electron impact on O2

    Erdman, P. W.; Zipf, E. C.

    1987-01-01

    Electron impact on O2 has been employed to ascertain the absolute cross-section value and emission linewidths of the OI (3s 5S0-3p 5P; 7774 A) multiplet. The emission linewidths are highly Doppler-broadened in dissociative excitation, and display two distinct kinetic energy distributions: which indicate that both purely repulsive and discrete, bound, excited molecular states, which then predissociate, are involved in the dissociation process that leads to the excitation of OI 7774 A. The magnitude of the measured cross-section and the fragment kinetic energy distribution both indicate that the previous time-of-flight studies of the metastable OI (5S0) state require reinterpretation.

  17. Laser-induced fluorescence and polarized light in the collision regime: the He(2s 3S → 4p 3P) case

    Laser-induced fluorescence experiments carried out using linearly polarized photons from a pulsed laser on a He(2s 3S → 4p 3P) excitation-detection scheme in electrical discharges at 0.04-0.6 Torr, show that light emitted during the interaction and in the subsequent decay manifests anisotropy in its angular distribution and polarization. A rate equation approach is used to discuss the general features of the interaction between polarized light and atoms observed experimentally. The incident electromagnetic field is decomposed into multipolar components that may interact with the atom through an appropriate coupling. Defining the Einstein coefficients for each coupling, it is possible to introduce the equations for the dynamics of the atomic populations. For each direction and polarization, the temporal profile of the intensity during the transition is calculated. The theoretical prediction explains the outcome of the He experiment satisfactorily. (author)

  18. Photovoltaic effect of n-In_2O_3/p-Cu_2O heterojunction thin film cells

    NAKAZAWA, Tatsuo; KURANOUCHI, Shin'ichi

    1992-01-01

    Electrical and photovoltaic characteristics of n-In_2O_3/p-Cu_2O heterojunction thin film cells were investigated. Cu_2O semiconducting films were prepared by simple method of thermal oxidation of copper foil in air. Conversion efficiency of 0.57% was obtained under illumination of the sunlight. It is thought that a high series resistance of the diode, which originated from a interface between Cu_2O film and copper foil, causes the poor characteristics. Photovoltaic characteristics of the cel...

  19. Effects of non-adiabatic and Coriolis couplings on the bound states of He(2 ^3S)+He(2 ^3P)

    Cocks, Daniel G; Peach, Gillian

    2009-01-01

    The effects of non-adiabatic and Coriolis couplings on the bound states of the He(2 ^3S_1)+He(2 ^3P_j) system, where j=0,1,2, are investigated using the recently available ab initio short-range $^{1,3,5}\\Sigma^{+}_{g,u}$ and $^{1,3,5}\\Pi_{g,u}$ potentials computed by Deguilhem et al. (J. Phys. B: At. Mol. Opt. Phys. 42 (2009) 015102). Three sets of calculations have been undertaken: single-channel, multichannel without Coriolis couplings and full multichannel with Coriolis couplings. We find that non-adiabatic effects are negligible for 0^-_u,0^\\pm_g,1_u,2_g,3_g Hund case (c) sets of levels in the j=2 asymptote but can be up to 6% for some of the 0^+_u and 1_g sets of levels where near degeneracies are present in the single-channel diagonalized potentials. Coriolis couplings are most significant for weakly bound levels, ranging from 1-5% for total angular momenta J=1,2 and up to 10% for J=3. Levels near the j=1 and j=0 asymptotes agree closely with previous multichannel calculations based upon long-range pote...

  20. Two-step laser excitation of 4snd 3D1,2,3 and 4sns 3S1 states from the 4s4p 3P levels in zinc

    We present new experimental data on the term energies and quantum defects of the even-parity triplet states of zinc using a two-step laser excitation scheme in conjunction with a thermionic diode ion detector. The first laser was fixed at 32 501.399 cm-1 to populate the 4s4p 3P1 intermediate level. The 4s4p 3P0,2 fine structure components get populated through collisional energy transfer. The second laser was scanned covering the energy region 43 200 to 42 000 cm-1 revealing the highly excited states up to the first ionization limit. Our observations include 4snd 3D2 (14 ≤ n ≤ 55) and 4sns 3S1 (15 ≤ n ≤ 35) Rydberg series excited from the 4s4p 3P1 level. In addition, 4snd 3D3 (13 ≤ n ≤ 49) and 4snd 3D1 (10 ≤ n ≤ 20) series including few members of the 4sns 3S1 series have also been observed from the 4s4p 3P2 and 4s4p 3P0 levels, respectively. The binding energy of 4s4p 3P1 has been determined as 43 267.93 ± 0.02 cm-1, which consequently yields the first ionization potential of zinc as 75 769.35 ± 0.05 cm-1, which is in good agreement with that reported previously

  1. Influence of relaxation effects on probabilities of the 2s2p3 S2—2s2 2p2 3p1,2intercombination

    袁萍; 刘欣生; 等

    2003-01-01

    Transition probabilities of the 2s2p3 5S2-2s2 2P2 3P1,2 intercombination transitions in NII have been calculated by using a large-scale multiconfiguration Dirac-Fock method.In the calculation themost important effects of relativity,correlation,and relaxation are considered.From the calculated transition probabilities,the lifetime of the s22p3 5S2 metastable state is derived.The result is in excellent agreement agreement with the latest experimental result.In the meantime the influence of anomalously strong relaxation effects on probabilities of the 2s2p3 5S2-2s2 2p2 3P1,2 lines in NII have been found.

  2. Self-supported Cu3P nanowire arrays as an integrated high-performance three-dimensional cathode for generating hydrogen from water.

    Tian, Jingqi; Liu, Qian; Cheng, Ningyan; Asiri, Abdullah M; Sun, Xuping

    2014-09-01

    Searching for inexpensive hydrogen evolution reaction (HER) electrocatalysts with high activity has attracted considerable research interest in the past years. Reported herein is the topotactic fabrication of self-supported Cu3 P nanowire arrays on commercial porous copper foam (Cu3 P NW/CF) from its Cu(OH)2 NW/CF precursor by a low-temperature phosphidation reaction. Remarkably, as an integrated three-dimensional hydrogen-evolving cathode operating in acidic electrolytes, Cu3 P NW/CF maintains its activity for at least 25 hours and exhibits an onset overpotential of 62 mV, a Tafel slope of 67 mV dec(-1) , and a Faradaic efficiency close to 100 %. Catalytic current density can approach 10 mA cm(-2) at an overpotential of 143 mV. PMID:25044801

  3. 弛豫与关联效应对NII离子2s22p3s3P1-2s22p2 1D2与2s22p3s 1P1-2s22p2 3P0,1,2自旋禁戒跃迁概率的影响%Influence of relaxation and correlation effects on probabilities of the 2s22p3s 3P1-2s22p2 1D2 and 2s22p3s 1P1-2s22p2 3P0,1,2 intercombination transitions in NII

    袁萍; 刘欣生; 张义军; 颉录有; 董晨钟

    2003-01-01

    用多组态Dirac-Fock方法,并系统考虑相对论效应、电子关联、弛豫效应等重要贡献,计算了NII离子2s22p3s 3P1-2s22p2 1D2和2s22p3s 1P1-2s22p2 3P0,1,2自旋禁戒跃迁概率和振子强度.通过比较计算证实:弛豫和关联效应对禁戒跃迁概率的影响非常大,考虑了这些效应后,计算结果有显著的改善.由跃迁概率和振子强度的计算值推断,2s22p3s 3P1-2s22p2 1D2的谱线强度应该比原有的理论预言值小.

  4. Cu3P

    Villars, P.; Cenzual, K.; Daams, J.; Gladyshevskii, R.; Shcherban, O.; Dubenskyy, V.; Melnichenko-Koblyuk, N.; Pavlyuk, O.; Savysyuk, I.; Stoyko, S.; Sysa, L.

    This document is part of Subvolume A6 `Structure Types. Part 6: Space Groups (166) R-3m - (160) R3m' of Volume 43 `Crystal Structures of Inorganic Compounds' of Landolt-Börnstein - Group III `Condensed Matter'.

  5. Effects of non-adiabatic and Coriolis couplings on the bound states of He(2 3S)+He(2 3P)

    The effects of non-adiabatic and Coriolis couplings on the bound states of the He(2 3S1) + He(2 3Pj) system, where j = 0, 1, 2, are investigated using the recently available ab initio short-range 1,3,5Σ+g,u and 1,3,5Πg,u potentials computed by Deguilhem et al (2009 J. Phys. B: At. Mol. Opt. Phys. 42 015102). Three sets of calculations have been undertaken: single-channel, multichannel without Coriolis couplings and full multichannel with Coriolis couplings. We find that non-adiabatic effects are negligible for 0-u, 0±g, 1u, 2g, 2u, 3g Hund case (c) sets of levels in the j = 2 asymptote but can be up to 15% for some of the 0+u and 1g sets of levels where near degeneracies are present in the single-channel diagonalized potentials. Coriolis couplings are most significant for weakly bound levels, ranging from 1% to 5% for total angular momenta J = 1, 2 and up to 10% for J = 3. Levels near the j = 1 and j = 0 asymptotes agree closely with previous multichannel calculations based upon long-range potentials constructed from retarded resonance dipole and dispersion interactions. Assignment of theoretical levels to experimental observations using criteria based upon the short-range character of each level and their coupling to metastable ground states produces well-matched assignments for the majority of observations. After a 1% increase in the slope of the 5Σ+g,u and 5Πg,u input potentials near the classical turning point is applied, improved matching of previous assignments is obtained and further assignments can be made, reproducing very closely the number of experimental observations.

  6. Comparative study of structural and morphological properties of CuIn{sub 3}S{sub 5} and CuIn{sub 7}S{sub 11} materials

    Khemiri, N., E-mail: naoufel_khemiri@yahoo.f [Laboratoire de Photovoltaique et Materiaux Semi-conducteurs, ENIT BP 37, Le belvedere 1002-Tunis (Tunisia); Kanzari, M. [Laboratoire de Photovoltaique et Materiaux Semi-conducteurs, ENIT BP 37, Le belvedere 1002-Tunis (Tunisia)

    2010-02-15

    CuIn{sub 3}S{sub 5} and CuIn{sub 7}S{sub 11} powders were prepared by solid-state reaction method using high-purity elemental copper, indium and sulphur. The films prepared from CuIn{sub 3}S{sub 5} and CuIn{sub 7}S{sub 11} powders were grown by thermal evaporation under vacuum (10{sup -6} Torr) on glass substrates at different substrate temperature Ts varying from room temperature to 200 deg. C. The powders and thin films were characterized for their structural properties by using X-ray diffraction (XRD) and energy dispersive X-ray (EDX). Both powders were polycrystalline with chalcopyrite and spinel structure, respectively. From the XRD data, we calculated the lattice parameters of the structure for the compounds. For CuIn{sub 3}S{sub 5} powder, we also calculated the cation-anion bond lengths. The effect of substrate temperature Ts on the structural properties of the films, such as crystal phase, preferred orientation and crystallinity was investigated. Indeed, X-ray diffraction analysis revealed that the films deposited at a room temperature (30 deg. C) are amorphous in nature while those deposited on heated were polycrystalline with a preferred orientation along (1 1 2) of the chalcopyrite phase and (3 1 1) of the spinel phase for CuIn{sub 3}S{sub 5} and CuIn{sub 7}S{sub 11} films prepared from powders, respectively. The morphology of the films was determined by atomic force microscopy AFM. The surface roughness and the grain size of the films increase on increasing the substrate temperature.

  7. Cu{sub 6}Te{sub 3}S. A Cu-filled Cr{sub 3}Si-structure variant

    Giller, Malte; Grotz, Carolin; Nilges, Tom [Technische Universitaet Muenchen, Garching (Germany). Dept. of Chemistry; Rudyk, Brent W.; Mar, Arthur [Alberta Univ., Edmonton, AB (Canada). Dept. of Chemistry

    2014-07-01

    A solid state melting and annealing route was used to prepare Cu{sub 6}Te{sub 3}S, a copper telluride sulfide representing a filled variant of the Cr{sub 3}Si structure type. The title compound exhibits a reversible phase transition at 404 K which was confirmed by thermal analysis, temperature dependent X-ray single crystal and powder diffractometry. Both polymorphs crystallize cubic in space groups P anti 43n and P2{sub 1}3, respectively. X-ray photoelectron spectroscopy (XPS) was performed to evaluate the electronic structure of Cu{sub 6}Te{sub 3}S and to determine the oxidation state of Cu in the title compound.

  8. Nano-sized quaternary CuGa2In3S8 as an efficient photocatalyst for solar hydrogen production

    Kandiel, Tarek

    2014-09-03

    The synthesis of quaternary metal sulfide (QMS) nanocrystals is challenging because of the difficulty to control their stoichiometry and phase structure. Herein, quaternary CuGa2In3S8 photocatalysts with a primary particle size of ≈4nm are synthesized using a facile hot-injection method by fine-tuning the sulfur source injection temperature and aging time. Characterization of the samples reveals that quaternary CuGa2In3S8 nanocrystals exhibit n-type semiconductor characteristics with a transition band gap of ≈1.8eV. Their flatband potential is located at -0.56V versus the standard hydrogen electrode at pH6.0 and is shifted cathodically by 0.75V in solutions with pH values greater than 12.0. Under optimized conditions, the 1.0wt% Ru-loaded CuGa2In3S8 photocatalyst exhibits a photocatalytic H2 evolution response up to 700nm and an apparent quantum efficiency of (6.9±0.5)% at 560nm. These results indicate clearly that QMS nanocrystals have great potential as nano-photocatalysts for solar H2 production. © 2014 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

  9. Study of χ{sub b} meson production in pp collisions at √(s) = 7 and 8 TeV and observation of the decay χ{sub b} (3P) → Υ (3S

    Aaij, R. [Nikhef National Institute for Subatomic Physics, Amsterdam (Netherlands); Adeva, B. [Universidad de Santiago de Compostela (Spain); Adinolfi, M. [Bristol Univ. (United Kingdom). H.H. Wills Physics Lab.; and others

    2014-10-15

    A study of χ{sub b} meson production at LHCb is performed on proton-proton collision data, corresponding to 3.0 fb{sup -1} of integrated luminosity collected at centre-of-mass energies √(s) = 7 and 8 TeV. The fraction of Υ(nS) mesons originating from χ{sub b} decays is measured as a function of the Υ transverse momentum in the rapidity range 2.0 < y{sup Υ} < 4.5. The radiative transition of the χ{sub b} (3P) meson to Υ(3S) is observed for the first time. The χ{sub b1} (3P) mass is determined to be m{sub χ{sub b{sub 1{sub ({sub 3{sub P{sub )}}}}}}} = 10 511.3 ± 1.7 ± 2.5MeV/c{sup 2}, where the first uncertainty is statistical and the second is systematic. (orig.)

  10. Determination and analysis of dispersive optical constants of CuIn{sub 3}S{sub 5} thin films

    Khemiri, N., E-mail: naoufel_khemiri@yahoo.f [Laboratoire de Photovoltaique et Materiaux Semiconducteurs-ENIT, Universite Tunis, ElManar BP 37, Le belvedere, 1002 Tunis (Tunisia); Sinaoui, A.; Kanzari, M. [Laboratoire de Photovoltaique et Materiaux Semiconducteurs-ENIT, Universite Tunis, ElManar BP 37, Le belvedere, 1002 Tunis (Tunisia)

    2011-04-15

    CuIn{sub 3}S{sub 5} thin films were prepared from powder by thermal evaporation under vacuum (10{sup -6} mbar) onto glass substrates. The glass substrates were heated from 30 to 200 {sup o}C. The films were characterized for their optical properties using optical measurement techniques (transmittance and reflectance). We have determined the energy and nature of the optical transitions of films. The optical constants of the deposited films were determined in the spectral range 300-1800 nm from the analysis of transmission and reflection data. The Swanepoel envelope method was employed on the interference fringes of transmittance patterns for the determination of variation of refractive index with wavelength. Wemple-Di Domenico single oscillator model was applied to determine the optical constants such as oscillator energy E{sub 0} and dispersion energy E{sub d} of the films deposited at different substrate temperatures. The electric free carrier susceptibility and the ratio of the carrier concentration to the effective mass were estimated according to the model of Spitzer and Fan.

  11. A Novel Sr2CuInO3S p-type semiconductor photocatalyst for hydrogen production under visible light irradiation

    Yushuai Jia; Jingxiu Yang; Dan Zhao; Hongxian Han; Can Li

    2014-01-01

    A novel Sr2CuInO3S oxysulfide p-type semiconductor photocatalyst has been prepared by solid state reaction method and it exhibits intriguing visible light absorption properties with a bandgap of 2.3 eV. The p-type semiconductor character of the synthesized Sr2CuInO3S was confirmed by Hall efficient measurement and Mott-Schottky plot analysis. First-principles density functional theory calculations (DFT) and electrochem-ical measurements were performed to elucidate the electronic structure and the energy band locations. It was found that the as-synthesized Sr2CuInO3S photocatalyst has appreciate conduction and valence band positions for hydrogen and oxygen evolution, respectively. Photocat-alytic hydrogen production experiments under a visible light irradiation (λ>420 nm) were carried out by loading different metal and metal-like cocatalysts on Sr2CuInO3S and Rh was found to be the best one among the tested ones.

  12. Preparation of Cu2Sn3S7 Thin-Film Using a Three-Step Bake-Sulfurization-Sintering Process and Film Characterization

    Tai-Hsiang Lui

    2015-01-01

    Full Text Available Cu2Sn3S7 (CTS can be used as the light absorbing layer for thin-film solar cells due to its good optical properties. In this research, the powder, baking, sulfur, and sintering (PBSS process was used instead of vacuum sputtering or electrochemical preparation to form CTS. During sintering, Cu and Sn powders mixed in stoichiometric ratio were coated to form the thin-film precursor. It was sulfurized in a sulfur atmosphere to form CTS. The CTS film metallurgy mechanism was investigated. After sintering at 500°C, the thin film formed the Cu2Sn3S7 phase and no impurity phase, improving its energy band gap. The interface of CTS film is continuous and the formation of intermetallic compound layer can increase the carrier concentration and mobility. Therefore, PBSS process prepared CTS can potentially be used as a solar cell absorption layer.

  13. Bonding Quandary in the [Cu3S2](3+) Core: Insights from the Analysis of Domain Averaged Fermi Holes and the Local Spin

    Ponec, Robert; Ramos-Córdoba, E.; Salvador, P.

    2013-01-01

    Roč. 117, č. 9 (2013), s. 1975-1982. ISSN 1089-5639 R&D Projects: GA ČR GA203/09/0118 Grant ostatní: SMCT(ES) MAT2008-04834; SMCT(ES) CTQ2011-23441/BQU; SFPU(ES) AP2008-01231 Institutional support: RVO:67985858 Keywords : Cu3S2 core * dafh analysis * bonding quandary Subject RIV: CF - Physical ; Theoretical Chemistry Impact factor: 2.775, year: 2013

  14. Development of a tunable Fabry-Perot etalon-based near-infrared interference spectrometer for measurement of the HeI 2{sup 3}S-2{sup 3}P spectral line shape in magnetically confined torus plasmas

    Ogane, S.; Shikama, T., E-mail: shikama@me.kyoto-u.ac.jp; Hasuo, M. [Department of Mechanical Engineering and Science, Graduate School of Engineering, Kyoto University, Kyoto 615-8540 (Japan); Zushi, H. [Research Institute for Applied Mechanics, Kyushu University, Fukuoka 816-8580 (Japan)

    2015-10-15

    In magnetically confined torus plasmas, the local emission intensity, temperature, and flow velocity of atoms in the inboard and outboard scrape-off layers can be separately measured by a passive emission spectroscopy assisted by observation of the Zeeman splitting in their spectral line shape. To utilize this technique, a near-infrared interference spectrometer optimized for the observation of the helium 2{sup 3}S–2{sup 3}P transition spectral line (wavelength 1083 nm) has been developed. The applicability of the technique to actual torus devices is elucidated by calculating the spectral line shapes expected to be observed in LHD and QUEST (Q-shu University Experiment with Steady State Spherical Tokamak). In addition, the Zeeman effect on the spectral line shape is measured using a glow-discharge tube installed in a superconducting magnet.

  15. A facile synthesis of MInSe2 (M = Cu, Ag) via low temperature pyrolysis of single source molecular precursors, [(R3P)2MIn(SeCOAr)4

    Shamik Ghoshal; Liladhar B Kumbhare; Vimal K Jain; Gautam K Dey

    2007-04-01

    The reaction of KSeCOAr with InCl3 and [MCl(PR3)2] in benzene afforded bimetallic complexes, [(R3P)2MIn(SeCOAr)4] (PR3 = PEt3 or PPh3; M = Cu or Ag; Ar = –C6H5 (phenyl) or 4-MeC6H4 (tolyl)). The triethylphosphine complexes decomposed rapidly when M = Ag while slowly when M = Cu. All these complexes were characterized by elemental analysis, IR, UV-VIS, NMR (1H, 31P) spectral data. Pyrolysis in a furnace at 300°C gave tetragonal MInSe2 (M = Cu, Ag) structure. Solvothermal decomposition of [(PPh3)2CuIn(SeCOAr)4] in boiling ethylene glycol gave nanorods of CuInSe2 which were characterized by XRD, EDAX, SEM and TEM.

  16. 高剥离类镁等电子序列的磁偶极MI和电四极E2光谱跃迁理论研究%HIGHLY STRIPPED MAGNETIC DIPOLE M1 AND ELECTRIC QUADRUPOLE E2 TRANSITIONS IN THE 3s3p CONFIGURATION OF THE Mg-LIKE IONS

    易有根; 郑志坚; 唐永建; 朱正和

    2003-01-01

    利用全相对论性多组态Dirac-Fock广义平均能级方法,系统地计算了类镁离子3s3p 磁偶极M1 3 P2-3P1 和电四极E2 3 P2-3P0(Z=20~103)光谱跃迁的能级间隔、跃迁几率和振子强度.计算中考虑了原子核的有限体积效应,进行了高阶Breit修正和QED修正,所得到的能级间隔和最近的实验数据及理论计算值进行了比较.计算结果表明:高原子序数的高荷电离子的磁偶极矩M1和电四极矩E2跃迁几率和中性原子的电偶极E1的相当,在ICF和MCF高温激光等离子体中,磁偶极矩M1和电四极矩E2跃迁过程不容被忽视.

  17. Crystal momentum dependence of the correlation satellite intensity in the 3p → 3d resonant photoemission spectra of Bi2Sr2CaCu2O8 + δ

    Goldoni, A.; Corradini, V.; del Pennino, U.; Sangalli, P.; Parmigiani, F.; Avila, J.; Teodorescu, C.

    2000-05-01

    Angle-resolved resonant photoemission measurements at the Cu3pCu3d threshold have been performed on the superconducting cuprate Bi2Sr2CaCu2O8 + δ. We have investigated in particular the correlation satellite appearing in the valence band photoemission spectrum to investigate the effect of solid state on the interference effect occurring at resonance. We found that the intensity of the correlation satellite changes with the electron take-off angle in a way that depends on the particular crystallographic direction and on the sample hole doping. These results indicate that the intensity enhancement at the absorption edge is a real resonance albeit the intermediate state in the autoionization process is partly delocalised. This fact does not prevent the occurrence of interference between indirect and direct photoemission.

  18. Crystal momentum dependence of the correlation satellite intensity in the 3p {yields} 3d resonant photoemission spectra of Bi{sub 2}Sr{sub 2}CaCu{sub 2}O{sub 8+{delta}}

    Goldoni, A. [INFM, Trieste (Italy); Corradini, V.; Del Pennino, U. [INFM, Modena (Italy); Sangalli, P. [INFM, Pavia (Italy); Parmigiani, F. [INFM, Brescia (Italy); Avila, J. [CSIC, Madrid (Spain). Inst. de Ciencia de Materiales; Laboratoire pour l' Utilisation du Rayonnement Electromagnetique (LURE), Paris-11 Univ., 91 - Orsay (France); Teodorescu, C. [Laboratoire pour l' Utilisation du Rayonnement Electromagnetique (LURE), Paris-11 Univ., 91 - Orsay (France)

    2000-05-01

    Angle-resolved resonant photoemission measurements at the Cu3p {yields} Cu3d threshold have been performed on the superconducting cuprate Bi{sub 2}Sr{sub 2}CaCu{sub 2}O{sub 8+{delta}}. We have investigated in particular the correlation satellite appearing in the valence band photoemission spectrum to investigate the effect of solid state on the interference effect occurring at resonance. We found that the intensity of the correlation satellite changes with the electron take-off angle in a way that depends on the particular crystallographic direction and on the sample hole doping. These results indicate that the intensity enhancement at the absorption edge is a real resonance albeit the intermediate state in the autoionization process is partly delocalised. This fact does not prevent the occurrence of interference between indirect and direct photoemission. (orig.)

  19. Crystal momentum dependence of the correlation satellite intensity in the 3p → 3d resonant photoemission spectra of Bi2Sr2CaCu2O8+δ

    Angle-resolved resonant photoemission measurements at the Cu3pCu3d threshold have been performed on the superconducting cuprate Bi2Sr2CaCu2O8+δ. We have investigated in particular the correlation satellite appearing in the valence band photoemission spectrum to investigate the effect of solid state on the interference effect occurring at resonance. We found that the intensity of the correlation satellite changes with the electron take-off angle in a way that depends on the particular crystallographic direction and on the sample hole doping. These results indicate that the intensity enhancement at the absorption edge is a real resonance albeit the intermediate state in the autoionization process is partly delocalised. This fact does not prevent the occurrence of interference between indirect and direct photoemission. (orig.)

  20. A structural comparison of two thallium copper erbium sulfides. TlCu{sub 3}Er{sub 2}S{sub 5} and Tl{sub 2}Cu{sub 5}Er{sub 3}S{sub 8}

    Eberle, Marcel A.; Schleid, Thomas [Univ. of Stuttgart (Germany). Inst. of Inorganic Chemistry; Babo, Jean-Marie [Univ. of Notre Dame, IN (United States). Dept. of Civil Engineering and Geological Sciences and Dept. of Chemistry and Biochemistry

    2014-08-15

    Orange TlCu{sub 3}Er{sub 2}S{sub 5} crystallizes in the orthorhombic space group Cmcm (a = 391.27(2), b = 1382.91(7), c = 1630.54(8) pm, Z = 4). Its crystal structure contains one Tl{sup +}, one Er{sup 3+}, two Cu{sup +}, and three S{sup 2-} ions as crystallographically unique components. All Cu{sup +} cations are coordinated by four S{sup 2-} anions to form [CuS{sub 4}]{sup 7-} tetrahedra, which have vertex- and edge-connectivity to build up {sub ∞}{sup 2}{[Cu_3S_5]"7"-} layers parallel to the (010) plane. The Er{sup 3+} cations are octahedrally surrounded by six S{sup 2-} anions. These [ErS{sub 6}]{sup 9-} units share trans-oriented edges forming linear chains, which are further linked by common vertices yielding {sub ∞}{sup 1}{[Er_2S_1_0]"1"4"-} double strands. Further fusion via common vertices results in {sub ∞}{sup 2}{[Er_2S_5]"4"-} layers parallel to the (010) plane. Alternatingly stacked along [010] and condensed via S{sup 2-} anions, these two types of layers form a three-dimensional framework, leaving tunnels along [100], where the Tl{sup +} cations fit in. These are each coordinated by eight S{sup 2-} anions in the shape of bicapped trigonal prisms. Tl{sub 2}Cu{sub 5}Er{sub 3}S{sub 8} was obtained as black single crystals with metallic luster (monoclinic, Cm, a = 1381.69(7), b = 390.73(2), c = 1435.98(7) pm, β =111.132(3) {sup circle}, Z = 2). Four of the five crystallographically different Cu{sup +} cations are tetrahedrally surrounded by S{sup 2-} anions, whereas (Cu3){sup +} is situated in sulfur triangles. Connected via common vertices and edges, the copper-sulfur polyhedra form strongly corrugated {sub ∞}{sup 2}{[Cu_5S_8]"1"1"-} layers parallel to the (20 anti 1) plane. All Er{sup 3+} cations are again coordinated by six S{sup 2-} anions in the shape of [ErS{sub 6}]{sup 9-} octahedra. Their condensation via edges and vertices leads to {sub ∞}{sup 2}{[Er_3S_8]"7"-} layers spreading out parallel to the (010) plane. Both types of anionic

  1. 3p deletion syndrome.

    Kaur, Anupam; Khetarpal, S

    2013-08-01

    3p deletion is a rare cytogenetic finding. Here we describe a 3 months old male with congenital malformations. His karyotype revealed 3p deletion 46,XY,del(3)(p25-pter). The child had flexion deformity of wrist and elbow which has never been reported before. PMID:24036645

  2. On the kinetic and thermodynamic fragility of the Pt{sub 60}Cu{sub 16}Co{sub 2}P{sub 22} and Pt{sub 57.3}Cu{sub 14.6}Ni{sub 5.3}P{sub 22.8} bulk metallic glasses

    Gallino, Isabella, E-mail: i.gallino@mx.uni-saarland.de [Saarland University, Department of Materials Science and Engineering, Campus C6.3, 66123 Saarbruecken (Germany); Gross, Oliver [Saarland University, Department of Materials Science and Engineering, Campus C6.3, 66123 Saarbruecken (Germany); Dalla Fontana, Giulia [Department of Chemistry IFM and NIS, University of Torino, V. Giuria 7, 10125 Torino (Italy); Evenson, Zach; Busch, Ralf [Saarland University, Department of Materials Science and Engineering, Campus C6.3, 66123 Saarbruecken (Germany)

    2014-12-05

    Highlights: • The studied Pt–Cu–(Ni,Co)–P glasses are more fragile than Zr-based alloys. • They show large increases in the C{sub p} at T{sub g} and small barriers for cooperative rearrangements of atoms. • They have fragility parameters among the lowest reported for BMG systems (D{sup *} = 10–12). • They crystallize into a state that melts with distinctly high entropy of fusion. • The microscopic origin of their fragility seems different than that for Zr- and Pd-based BMGs. - Abstract: The investigations in this study focus on bulk metallic glass (BMG) alloy families based on noble metals like Pt, which are more kinetically fragile than Zr-based BMG systems. Thermophysical properties have been investigated by calorimetry and thermal mechanical analyses for the determination of the specific heat capacity and viscosity, respectively. For the Pt{sub 60}Cu{sub 16}Co{sub 2}P{sub 22} and Pt{sub 57.3}Cu{sub 14.6}Ni{sub 5.3}P{sub 22.8} BMG compositions consistent Vogel–Fulcher–Tammann (VFT) fits of the viscosity measurements are established, and the temperature dependence of the configurational entropy is calculated from thermodynamic data. Fits to the Adam–Gibbs equation are performed using this configurational entropy change. Their fragile nature is compared to that of Zr-based alloys in terms of structural considerations.

  3. Transition probability values of the 1s22s3p 3P0 level in Be-like ions

    Transition probability values from the 1s22s3p 3P0 level for selected beryllium-like ions, from Z = 5 to 92, are calculated using the multi-configuration Dirac–Fock method including QED corrections, and full correlation up to the 4f subshell in both initial and final levels, for 1s22s3s 3S1, 1s22s2p 3P2 level and 1s22p23P1 decay modes of this level. (paper)

  4. Fine-structure energy levels, oscillator strengths and lifetimes in Cu XVI

    Gupta, G P [Department of Physics, S D (Postgraduate) College, Muzaffarnagar-251 001 (Affiliated to Chowdhary Charan Singh University, Meerut-250 004) (India); Msezane, A Z, E-mail: g_p_gupta1@yahoo.co.in [Department of Physics and Center for Theoretical Studies of Physical Systems, Clark Atlanta University, Atlanta, GA 30314 (United States)

    2011-05-01

    We have performed large-scale CIV3 calculations of excitation energies from ground state for 69 fine-structure levels as well as of oscillator strengths and radiative decay rates for all electric-dipole-allowed and intercombination transitions among the fine-structure levels of the terms belonging to the (1s{sup 2}2s{sup 2}2p{sup 6})3s{sup 2}3p{sup 2}, 3s3p{sup 3}, 3p{sup 4}, 3s{sup 2}3p3d, 3s{sup 2}3p4s, 3s{sup 2}3p4p, 3s{sup 2}3p4d, and 3s{sup 2}3p4f configurations of Cu XVI. These states are represented by very extensive configuration-interaction (CI) wave functions obtained with the computer code CIV3 of Hibbert. The important relativistic effects in intermediate coupling are incorporated by means of the Breit-Pauli Hamiltonian. Small adjustments to the diagonal elements of the Hamiltonian matrices have been made so that the energy splittings are as close as possible to the energy values of those from the National Institute for Standards and Technology. The mixing among several fine-structure levels is found to be very strong. From our radiative decay rates we have also calculated radiative lifetimes of the fine-structure levels. Our calculated lifetime for the high spin level 3s3p{sup 3}({sup 5}S{sub 2}) is found to be in excellent agreement with the experimental value of Trabert et al (1988 J. Opt. Soc. Am. B 5 2173). In this calculation, we also predict new data for several fine-structure levels where no other theoretical and/or experimental results are available.

  5. Relativistic atomic data for Cu-like tungsten

    Safronova, U. I.; Safronova, A. S.; Beiersdorfer, P.

    2013-05-01

    Energy levels, radiative transition probabilities, and autoionization rates for [Ne] 3s2 3p6 3d9 4l' nl , [Ne] 3s2 3p5 3d10 4l' nl (n=4-6), and [Ne] 3s2 3p6 3d9 5l' nl ,(n=5-7) states in Cu-like tungsten (W45+) are calculated using the relativistic many-body perturbation theory method (RMBPT code), the multiconfiguration relativistic Hebrew University Lawrence Livermore Atomic Code (HULLAC code), and the Hartree-Fock-relativistic method (COWAN code). Branching ratios relative to the first threshold and intensity factors are calculated for satellite lines, and dielectronic recombination (DR) rate coefficients are determined for the singly excited, as well as doubly excited non-autoionizing states in Cu-like W45+ ion. Contributions from the autoionizing doubly excited states (with n up to 500), which are particulary important for calculating total DR rates, are estimated. Synthetic dielectronic satellite spectra from Cu-like W are simulated in a broad spectral range from 3 to 70 Å. These calculations provide highly accurate values for a number of W45+ properties useful for a variety of applications including for fusion applications. This research was sponsored by the grant DE-FG02-08ER54951.

  6. Energy and Auger Widths of Triply Excited 3p3p3p 2po State of Lithium

    苟秉聪; 俞开智

    2003-01-01

    The high-lying triply excited 3p3p3p 2po state of the double hollow lithium atom is studied by using the saddlepoint complex-rotation method. The energy and Auger widths of this resonance are calculated. The relativistic corrections and mass polarization are included. The total Auger width is obtained by coupling the important open channels and summing over the other channels. The oscillator strength is also calculated. The results are compared with other theoretical and experimental data in the literature.

  7. Investigation of the ({radical}3 x {radical}3)R30{sup o}-Cu{sub 2}Si/Cu(1 1 1) surface alloy using DFT

    Shuttleworth, I.G., E-mail: shuttleworth.ian@gmail.com [Jubail University College, Jubail Industrial City, 31961 (Saudi Arabia)

    2011-05-15

    The electronic structure of the FCC, HCP and 2-fold bridge phases of the ({radical}3 x {radical}3)R30{sup o}-Cu{sub 2}Si/Cu(1 1 1) surface alloy have been investigated using LCAO-DFT. Analysis of the total electron density, partial density-of-states (PDOS) and crystal orbital overlap population (COOP) curves for the system have shown a surprising similarity between the intra- and inter-layer Si-Cu bond for each phase. Low hybridization between the Si 3s and 3p orbitals results in a low directionality of the Si-Cu bond within each of phase. The Si 3s orbitals are shown to form covalent bonds with their surrounding Cu atoms whereas the Si 3p and 3d orbitals are shown to form combinations of covalent and metallic bonds. The Si-Cu interaction is shown clearly to extend to the second layer of the alloy in deference to previous studies of Si/Cu alloys.

  8. Thermoelastic properties of Zn3P2

    Gerward, Leif; Olsen, J. Staun; Waśkowska, A.

    2011-01-01

    The bulk modulus and thermal expansion of Zn3P2 has been investigated at pressures up to 21GPa and temperatures down to 100K. The experimental zero-pressure bulk modulus is 80.7 ± 1.8GPa, in accordance with the bulk modulus scaling and lattice properties of the related compound Cd3P2. A tetragonal...... to orthorhombic phase transformation occurs above 11GPa with a relative volume change of-7.1%. Values for the thermal expansion coefficient are reported at 293, 200 and 100K....

  9. Photoelectron diffraction of magnetic ultrathin films: Fe/Cu(001)

    Tobin, J.G. (Lawrence Livermore National Lab., CA (USA)); Wagner, M.K. (Wisconsin Univ., Madison, WI (USA). Dept. of Chemistry); Guo, X.Q.; Tong, S.Y. (Wisconsin Univ., Milwaukee, WI (USA). Dept. of Physics)

    1991-01-03

    The preliminary results of an ongoing investigation of Fe/Cu(001) are presented here. Energy dependent photoelectron diffraction, including the spin-dependent variant using the multiplet split Fe3s state, is being used to investigate the nanoscale structures formed by near-monolayer deposits of Fe onto Cu(001). Core-level photoemission from the Fe3p and Fe3s states has been generated using synchrotron radiation as the tunable excitation source. Tentatively, a comparison of the experimental Fe3p cross section measurements with multiple scattering calculations indicates that the Fe is in a fourfold hollow site with a spacing of 3.6{Angstrom} between it and the atom directly beneath it, in the third layer. This is consistent with an FCC structure. The possibility of utilizing spin-dependent photoelectron diffraction to investigate magnetic ultrathin films will be demonstrated, using our preliminary spectra of the multiplet-split Fe3s os near-monolayer Fe/Cu(001). 18 refs., 10 figs.

  10. Absolute frequency measurement of the magnesium intercombination transition $^1S_0 \\to ^3P_1$

    Friebe, Jan; Pape, André; Riedmann, Matthias; Moldenhauer, Karsten; Mehlstäubler, Tanja; Rehbein, Nils; Lisdat, Christian; Rasel, Ernst M.; Ertmer, Wolfgang; Schnatz, Harald; Lipphardt, Burghard; Grosche, Gesine

    2007-01-01

    We report on a frequency measurement of the $(3s^2)^1S_0\\to(3s3p)^3P_1$ clock transition of $^{24}$Mg on a thermal atomic beam. The intercombination transition has been referenced to a portable primary Cs frequency standard with the help of a femtosecond fiber laser frequency comb. The achieved uncertainty is $2.5\\times10^{-12}$ which corresponds to an increase in accuracy of six orders of magnitude compared to previous results. The measured frequency value permits the calculation of several ...

  11. Atomic scattering in the diffraction limit: electron transfer in keV Li+-Na(3s, 3p) collisions

    Poel, Mike van der; Nielsen, C.V.; Rybaltover, M.;

    2002-01-01

    We measure angle differential cross sections (DCS) in Li+ + Na --> Li + Na+ electron transfer collisions in the 2.7-24 keV energy range. We do this with a newly constructed apparatus which combines the experimental technique of cold target recoil ion momentum spectroscopy with a laser-cooled target...... quantum scattering amplitudes are derived by the eikonal method. The resulting angle-differential electron transfer cross sections and their diffraction patterns agree with the experimental level-to-level results over most scattering angles in the energy range....

  12. BOREAS Level-3p Landsat TM Imagery: Geocoded and Scaled At-sensor Radiance

    Nickeson, Jaime; Knapp, David; Newcomer, Jeffrey A.; Hall, Forrest G. (Editor); Cihlar, Josef

    2000-01-01

    For BOReal Ecosystem-Atmosphere Study (BOREAS), the level-3p Landsat Thematic Mapper (TM) data were used to supplement the level-3s Landsat TM products. Along with the other remotely sensed images, the Landsat TM images were collected in order to provide spatially extensive information over the primary study areas. This information includes radiant energy, detailed land cover, and biophysical parameter maps such as Fraction of Photosynthetically Active Radiation (FPAR) and Leaf Area Index (LAI). Although very similar to the level-3s Landsat TM products, the level-3p images were processed with ground control information, which improved the accuracy of the geographic coordinates provided. Geographically, the level-3p images cover the BOREAS Northern Study Area (NSA) and Southern Study Area (SSA). Temporally, the four images cover the period of 20-Aug-1988 to 07-Jun-1994. Except for the 07-Jun-1994 image, which contains seven bands, the other three contain only three bands.

  13. Comparative investigation of the c(2 Multiplication-Sign 2)-Si/Cu(0 1 1) and ({radical}3 Multiplication-Sign {radical}3)R30 Degree-Sign -Cu{sub 2}Si/Cu(1 1 1) surface alloys using DFT

    Shuttleworth, I.G., E-mail: shuttleworth.ian@gmail.com [Jubail University College, Jubail Industrial City 31961 (Saudi Arabia)

    2012-02-01

    The electronic structure of the c(2 Multiplication-Sign 2)-Si/Cu(0 1 1) surface alloy has been investigated and compared to the structures seen in the three phases of the ({radical}3 Multiplication-Sign {radical}3)R30 Degree-Sign Cu{sub 2}Si/Cu(1 1 1) system, using LCAO-DFT. The weighted surface energy increase between the alloyed Cu(0 1 1) and Cu(1 1 1) surfaces is 126.7 meV/Si atom. This increase in energy for the (0 1 1) system when compared to the (1 1 1) system is assigned to the transition from a hexagonal to a rectangular local bonding environment for the Si ion cores, with the hexagonal environment being energetically more favorable. The Si 3s state is shown to interact covalently with the Cu 4s and 4p states whereas the Si 3p state, and to a lesser extent the Si 3d state, forms a mixture of covalent and metallic bonds with the Cu states. The Cu 4s and 4p states are shown to be altered by approximately the same amount by both the removal of Cu ion cores and the inclusion of Si ion cores during the alloying of the Cu(0 1 1) surface. However, the Cu 3d states in the surface and second layers of the alloy are shown to be more significantly altered during the alloying process by the removal of Cu ion cores from the surface layer rather than by the addition of Si ion cores. This is compared to the behavior of the Cu 3d states in the surface and second layers of the each phase of the ({radical}3 Multiplication-Sign {radical}3)R30 Degree-Sign -Cu{sub 2}Si/Cu(1 1 1) alloy and consequently the loss of Cu-Cu periodicity during alloying of the Cu(0 1 1) surface is conjectured as the driving force for changes to the Cu 3d states. The accompanying changes to the Cu 4s and 4p states in both the c(2 Multiplication-Sign 2)-Si/Cu(0 1 1) and ({radical}3 Multiplication-Sign {radical}3)R30 Degree-Sign -Cu{sub 2}Si/Cu(1 1 1) alloys are quantified and compared. The study concludes with a brief quantitative study of changes in the bond order of the Cu-Cu bonds during alloying of

  14. $^3P_2$ Superfluids Are Topological

    Mizushima, Takeshi

    2016-01-01

    We clarify the topology of the $^3P_2$ superfluidity which is expected to be realized in the cores of neutron stars and cubic odd-parity superconductors. The phase diagram includes the unitary uniaxial/biaxial nematic phases and nonunitary ferromagnetic and cyclic phases. We here show that the low-energy structures of all the phases are governed by different types of topologically protected gapless fermionic excitations: Surface Majorana fermions in nematic phases, single itinerant Majorana fermion in the ferromagnetic phase, and a quartet of itinerant Majorana fermions in the cyclic phase. Using the superfluid Fermi liquid theory, we also demonstrate that dihedral-two and -four biaxial nematic phases are thermodynamically favored in the weak coupling limit under a magnetic field. The mass acquisition of surface Majorana fermions in nematic phases is subject to symmetry.

  15. Crystal structure of ∼RCu3S3 and ∼RCuTe2 (R=Gd-Lu) compounds

    Gulay, L. D.; Daszkiewicz, M.; Shemet, V. Ya.

    2012-02-01

    The crystal structures of ternary compounds TbCu3S3, Dy1.06Cu2.84S3 (space group R3¯), Ho0.67Cu2S2 (space group P3¯m1), ErCu3S3 (space group P3¯1c), Yb0.80Cu1.60S2, Lu0.67Cu2S2, TbCuTe2, DyCuTe2, Tm1.07Cu0.78Te2, LuCuTe2 (space group P3¯m1), Gd0.75Cu1.74Te2 (space group P3¯1m) were determined by means of X-ray single crystal diffraction. The S(Te) atoms are stacked in a close packed arrangement with the layers in the sequence AB. The R atoms are distributed over octahedral interstices whereas Cu atoms are located in tetrahedral interstices. Disorder of R and Cu atoms in studied chalcogenides is found. Crystal structure comparison showed that TbCuTe2 and DyCuTe2 crystallize as superstructure 2a×2a×2c to CaAl2Si2 structure type, whereas Gd0.75Cu1.74Te2, ErCu3S3 and TbCu3S3 (Dy1.06Cu2.84S3) have superstructure √3a×√3a×nc with n=1, 2, 3.

  16. Fine-structure energy levels, oscillator strengths and lifetimes in Cu XVI

    We have performed large-scale CIV3 calculations of excitation energies from ground state for 69 fine-structure levels as well as of oscillator strengths and radiative decay rates for all electric-dipole-allowed and intercombination transitions among the fine-structure levels of the terms belonging to the (1s22s22p6)3s23p2, 3s3p3, 3p4, 3s23p3d, 3s23p4s, 3s23p4p, 3s23p4d, and 3s23p4f configurations of Cu XVI. These states are represented by very extensive configuration-interaction (CI) wave functions obtained with the computer code CIV3 of Hibbert. The important relativistic effects in intermediate coupling are incorporated by means of the Breit-Pauli Hamiltonian. Small adjustments to the diagonal elements of the Hamiltonian matrices have been made so that the energy splittings are as close as possible to the energy values of those from the National Institute for Standards and Technology. The mixing among several fine-structure levels is found to be very strong. From our radiative decay rates we have also calculated radiative lifetimes of the fine-structure levels. Our calculated lifetime for the high spin level 3s3p3(5S2) is found to be in excellent agreement with the experimental value of Trabert et al (1988 J. Opt. Soc. Am. B 5 2173). In this calculation, we also predict new data for several fine-structure levels where no other theoretical and/or experimental results are available.

  17. Helium 3 3S decay rates in a high-pressure afterglow

    We report a total collisional quenching rate of (6.4 +- 0.3) x 10-12 cm3 sec-1 at 292 0K (or a thermally averaged cross section of 0.36 x 10-16 cm2) for He 3 3S atoms colliding with ground-state He atoms. This rate is determined by using a pulsed dye laser to populate the 3 3S level in a He aftergow and then observing the decay of the 3 3S → 2 3P fluorescence. We see no evidence for three-body collisional quenching of 3 3S atoms at pressures up to 300 Torr

  18. Irradiation-induced softening of Ni3P and (Ni, Fe, Cr)3P alloys

    Production of amorphous alloys by solid state reactions (SSR) has attracted much interest during the last few years. One of the methods to induce such a reaction is the irradiation of suitable crystalline alloys by fast particles. Examination of this kind of SSR in M3P type of brazing alloys (M: Metal) is attractive because of the following reason: In brazed joints of candidate structural materials like 316L stainless steel for applications in fusion reactors, crystalline intermetallic phases have been detected which are unstable relative to the amorphous state when irradiated at moderate temperatures with fast particles. It is expected that the transition to the amorphous state is accompanied by changes of the mechanical properties, which are of fundamental interest in this context. Until now, only a few studies on the evolution of mechanical properties during amorphization have been performed. Measurements of microhardness of the crystalline and the corresponding amorphous phase do not exist to the authors knowledge. In this communication, the authors present results on changes of microhardness, due to amorphization by fast ions. The measurements have been performed on a model alloy Ni3P and on the brazed joint of stainless steel 316L, containing M3P (M: Ni, Fe, Cr) as one of the phases. Though microhardness is not a fundamental property of materials, it is a manifestation of several related properties, such as yield stress, ductility, work-hardening, elastic modulus and residual stress states. It represents a resistance for indentation and is, therefore, appropriate for comparative purposes

  19. Spectra and oscillator strengths of 3p63d9-3p53d10 and 3p63d9-3p63d84p transitions for cobalt-like Sn23+ ion

    Chen Ming-Lun; Yu Xiao-Guang

    2009-01-01

    This paper calculates the spectra and oscillator strengths for highly ionized cobalt-like Sn23+ ions 3p63d9-3p53d10,3p63d9 - 3p63d84p transitions by using a multi-configuration self-consistent field method program together with the proposed fitting formula. The calculations have a good agreement with observations.

  20. Photoemission time-delay measurements and calculations close to the 3s ionization minimum in Ar

    Guenot, D; Arnold, C L; Kroon, D; Dahlstrom, J M; Miranda, M; Fordell, T; Gisselbrecht, M; Johnsson, P; Mauritsson, J; Lindroth, E; Maquet, A; Taieb, R; L'Huillier, A; Kheifets, A S

    2012-01-01

    We present experimental measurements and theoretical calculations of photoionization time delays from the $3s$ and $3p$ shells in Ar in the photon energy range of 32-42 eV. The experimental measurements are performed by interferometry using attosecond pulse trains and the infrared laser used for their generation. The theoretical approach includes intershell correlation effects between the 3s and 3p shells within the framework of the random phase approximation with exchange (RPAE). The connection between single-photon ionization and the two-color two-photon ionization process used in the measurement is established using the recently developed asymptotic approximation for the complex transition amplitudes of laser-assisted photoionization. We compare and discuss the theoretical and experimental results especially in the region where strong intershell correlations in the 3s to kp channel lead to an induced "Cooper" minimum in the 3s ionization cross-section.

  1. Differential cross section of metastable Ne(3P0 and 3P2) scattered from ground state neon

    The differential elastic cross section for metastable Ne(3P0 and 3P2) from ground state Ne at collision energies between 70 and 150 meV have been measured. With a CW-dye laser it was possible to separate the cross sections for Ne(3P0) + Ne and Ne(3P2) + Ne and for the energy exchange process 20Ne* + 22Ne → 20Ne + 22Ne*. (Auth.)

  2. Differential cross section for Ne(3P0) and Ne(3P2) scattered from ground state neon

    The differential elastic cross sections for electronically excited Ne(3P0) and Ne(3P2) from ground state neon atoms at thermal collision energies have been measured separately. Potentials for Ne(3P0)+Ne could be determined and the height of the intermediate potential maxima for Ne(3P2)+Ne could be estimated to 25 meV. By preparing Ne(3P2) in special Msub(J) states scattering in single Ω molecular states could be observed. (Auth.)

  3. Differential cross section for Ne(3P0) and Ne(3P2) scattered from ground state neon

    The differential elastic cross sections for electronically exited Ne(3P0) and Ne(3P2) from ground state neon atoms at thermal collision energies have been measured separately. Potentials for Ne(3P0)+Ne could be determined and the height of the intermediate potential maxima for Ne(3P2)+Ne could be estimated to 25 meV. By preparing Ne(3P2) in special Msub(J) states scattering in single Ω molecular states could be observed. (Author)

  4. Resonant inverse photoemission study of late transition metals at 3p absorption edge

    Full text: Resonant inverse photoemission spectra (RIPES) of late transition metals (TM) were observed near TM 3p absorption edge. The RIPES spectra of polycrystalline Co, Ni and Cu, as well as single crystal Ni, were observed. Figure 1 shows resonant IPES spectra of polycrystalline Co, Ni and Cu, which were prepared by evaporation. These spectra ware excited by energy above 3p absorption edge (off-resonance). Since a core hole is created by these energies, TM 3d → 3p fluorescence peak is observed in each spectrum at high energy, which is indicated by vertical bars. The main peak just above EF is TM 3d structure, while TM 4sp is observed at 10 ∼ 15 eV. In resonant spectra, the 3d structure changes its intensity, while the 4sp structure does not. In case of Ni metal, satellite structures are also observed at about 2 and 4 eV. From a calculation by Tanaka and Jo, which is based on the Anderson impurity model, the observation of satellite structures suggests the 10 ∼ 20 % 3d8 in ground state The RIPES spectra in this study give us a direct evidence of 3d8 component in Ni metal

  5. Absolute frequency measurement of the magnesium intercombination transition $^1S_0 \\to ^3P_1$

    Friebe, Jan; Riedmann, Matthias; Moldenhauer, Karsten; Mehlstäubler, Tanja; Rehbein, Nils; Lisdat, Christian; Rasel, Ernst M; Ertmer, Wolfgang; Schnatz, Harald; Lipphardt, Burghard; Grosche, Gesine

    2007-01-01

    We report on a frequency measurement of the $(3s^2)^1S_0\\to(3s3p)^3P_1$ clock transition of $^{24}$Mg on a thermal atomic beam. The intercombination transition has been referenced to a portable primary Cs frequency standard with the help of a femtosecond fiber laser frequency comb. The achieved uncertainty is $2.5\\times10^{-12}$ which corresponds to an increase in accuracy of six orders of magnitude compared to previous results. The measured frequency value permits the calculation of several other optical transitions from $^1S_0$ to the $^3P_J$-level system for $^{24}$Mg, $^{25}$Mg and $^{26}$Mg. We describe in detail the components of our optical frequency standard like the stabilized spectroscopy laser, the atomic beam apparatus used for Ramsey-Bord\\'e interferometry and the frequency comb generator and discuss the uncertainty contributions to our measurement including the first and second order Doppler effect. An upper limit of $3\\times10^{-13}$ in one second for the short term instability of our optical f...

  6. Absence of hydrogen in superconducting molybdenum sulfide, Mo 3S 4

    Baillif, R.; Yvon, K.; Fischer, P.

    1983-09-01

    Superconducting Mo 3S 4( Tc=1.8 K) was prepared from the ternary sulfides MMo 3S 4 ( M=Cu, Ni) by the acid extraction method, and was studied by neutron diffraction and NMR spectroscopy. In contrast to earlier reports no significant amounts of hydrogen could be found in the rhombohedral structure. However, large proton concentrations were found in samples which had been exposed to moist air.

  7. Absence of hydrogen in superconducting molybdenum sulfide, Mo3S4

    Superconducting Mo3S4 (Tsub(c)=1.8 K) was prepared from the ternary sulfides MMo3S4 (M = Cu, Ni) by the acid extraction method, and was studied by neutron diffraction and NMR spectroscopy. In contrast to earlier reports no significant amounts of hydrogen could be found in the rhombohedral structure. However, large proton concentrations were found in samples which had been exposed to moist air. (author)

  8. Is Y(4008) possibly a 1{sup --} ψ(3{sup 3}S{sub 1}) state?

    Chen, Li-Jin; Zhang, Ailin [Shanghai University, Department of Physics, Shanghai (China); Ye, Dan-Dan [Shanghai University, Department of Physics, Shanghai (China); Jiaxing University, College of Mathematics, Physics and Information Engineering, Jiaxing (China)

    2014-08-15

    The strong decays of the radially excited ψ(3{sup 3}S{sub 1}) state are studied within the 3P0 model. As a believed ψ(3{sup 3}S{sub 1}), some strong decay widths and relevant ratios of ψ(4040) are calculated in the model. In a similar way, as a possible ψ(3{sup 3}S{sub 1}), the same strong decay widths and relevant ratios of Y(4008) are presented. Our study indicates that Y (4008) is hard to be identified with a ψ(3{sup 3}S{sub 1}) charmonium once it is confirmed under the D{sup *} anti D{sup *} threshold, but it is possibly a ψ(3{sup 3}S{sub 1}) charmonium once it is confirmed above the D{sup *} anti D{sup *} threshold by experiment. (orig.)

  9. Cooling of Neutron Stars and 3P_2 neutron gap

    Grigorian, H.; Voskresensky, D.N.(National Research Nuclear University (MEPhI), Moscow, 115409, Russia)

    2005-01-01

    We study the dependence of the cooling of isolated neutron stars on the magnitude of the $3P_2$ neutron gap. It is demonstrated that our ``Nuclear medium cooling scenario'' is in favor of a suppressed value of the $3P_2$ neutron gap.

  10. 3p - 3d intershell interaction in Cr

    The photoemission of Cr films deposited under UHV conditions has been investigated in the photon energy range from 30 eV to 230 eV. The 3p - 3d intershell interaction gives rise to a strong maximum in the 3d partial yield above the 3p threshold. (orig.) 891 KBE/orig. 892 RDG

  11. Assessment of combined toxicity of heavy metals from industrial wastewaters on Photobacterium phosphoreum T3S

    Zeb, BibiSaima; Ping, Zheng; Mahmood, Qaisar; Lin, Qiu; Pervez, Arshid; Irshad, Muhammad; Bilal, Muhammad; Bhatti, Zulfiqar Ahmad; Shaheen, Shahida

    2016-02-01

    This research work is focusing on the toxicities of heavy metals of industrial origin to anaerobic digestion of the industrial wastewater. Photobacterium phosphoreum T3S was used as an indicator organism. The acute toxicities of heavy metals on P. phosphoreum T3S were assessed during 15-min half inhibitory concentration (IC50) as indicator at pH 5.5-6. Toxicity assays involved the assessment of multicomponent mixtures using TU and MTI approaches. The results of individual toxicity indicated that the toxicity of Cd, Cu and Pb on P. phosphoreum increased with increasing concentrations and there was a linear correlation. The 15-min IC50 values of Cd, Cu and Pb were 0.537, 1.905 and 1.231 mg/L, respectively, and their toxic order was Cd > Pb > Cu. The combined effects of Cd, Cu and Pb were assayed by equivalent concentration mixing method. The results showed that the combined effects of Cd + Cu, Cd + Pb, Cu + Pb, Cd + Cu + Pb were antagonistic, antagonistic and partly additive. The combined effect of three heavy metals was partly additive.

  12. The state dependence of the interaction of metastable rare gas atoms Rg sup * (ms sup 3 P sub 2 , sup 3 P sub 0 ) (Rg=Ne, Ar, Kr, Xe) with ground state sodium atoms

    Schohl, S.; Mueller, M.W.; Meijer, H.A.J.; Ruf, M.W.; Hotop, H. (Kaiserslautern Univ. (Germany, F.R.). Fachbereich Physik); Morgner, H. (Witten-Herdecke Univ., Witten (Germany, F.R.). Inst. fuer Experimentalphysik)

    1990-08-01

    Using crossed beams of metastable rare gas atoms Rg{sup *}(ms {sup 3}P{sub 2}, {sup 3}P{sub 0}) (Rg=Ne, Ar, Kr, Xe) and ground state sodium atoms Na(3s {sup 2}S{sub 1/2}), we have measured the energy spectra of electrons released in the respective Penning ionization processes at thermal collision energies. For Rg{sup *}({sup 3}P{sub 2})+Na(3s), the spectra are quite similar for the different rare gases, both in width and shape; they reflect attractive interactions in the entrance channel with well depths D{sub e}{sup *} (meV) decreasing slowly from Rg=Ne to Xe as follows: 676(18); 602(23); 565(26); 555(30). For Rg{sup *}({sup 3}P{sub 0})+Na(3 s), the spectra vary strongly with the rare gas, indicating a change in the character of the interaction from van der Waals type attraction (Ne) to chemical binding for Kr and Xe with well depths D{sub e}{sup *} (meV) of: 51(19); 107(25); 432(30); 530(50). These findings are explained through model calculations of the respective potential curves, in which the exchange and the spin orbit interaction in the excited rare gas and the molecular interaction between the two valence s-electrons in terms of suitably chosen singlet and triplet potentials are taken into account. These calculations also explain qualitatively the experimental finding that the ratios q{sub 2}/q{sub 0} of the ionization cross sections for Rg{sup *}({sup 3}P{sub 2})+Na and Rg{sup *}({sup 3}P{sub 0})+Na vary strongly with the rare gas from Ne to Xe as follows: 15.8(3.2); 2.6(4); 1.4(2); 1.6(4). (orig.).

  13. Chromosome 3p alterations in pancreatic endocrine neoplasia

    Amato, Eliana; Barbi, Stefano; Malpeli, Giorgio; Bersani, Samantha; Pelosi, Giuseppe; Capelli, Paola

    2010-01-01

    Pancreatic endocrine tumors (PET) are rare neoplasms classified as functioning (F-PET) or non-functioning (NF-PET) according to the presence of a clinical syndrome due to hormonal hypersecretion. PETs show variable degrees of clinical aggressiveness and loss of chromosome 3p has been suggested to be associated with an advanced stage of disease. We assessed chromosome 3p copy number in 113 primary PETs and 32 metastases by fluorescence in situ hybridization (FISH) using tissue microarrays. The series included 56 well-differentiated endocrine tumors (WDET), 62 well-differentiated endocrine carcinomas (WDEC), and 6 poorly differentiated endocrine carcinomas (PDEC). Chromosome 3p alterations were found in 23/113 (20%) primary tumors, with losses being predominant over gains (14% vs. 6%). Loss of 3p was found in 5/55 (9%) WDET, 11/52 (21%) WDEC, and never in PDEC. Gains of 3p were detected in 4/55 (7%) WDET, no WDEC, but notably in 3/6 (50%) PDEC (OR 23.6; P = 0.003). Metastases were more frequently monosomic for 3p compared to primary tumors (OR 3.6; P = 0.005). Monosomy was significantly associated with larger tumor size, more advanced tumor stage, and metastasis. No association was found with survival. Chromosome 3p copy number alterations are frequent events in advanced stage PET, with gains prevailing in PDEC while losses are more frequent in WDEC, supporting the view that a specific pattern of alterations are involved in these diverse disease subtypes. PMID:20981439

  14. Safety, Security and Safeguards (3S) Culture

    A meaningful discussion of Safety, Security, and Safeguards (3S) Culture requires a review of the concepts related to the culture of the three components. The concept of culture can be confusing, and so careful use of terminology is needed to enable a focused and constructive dialogue. To this end, this paper will use the concept of organizational culture as a backdrop for a broader discussion about how the three subcultures of safety, security and safeguards come together to enhance the mission of an organization. Since the accidents at Three Mile Island and Chernobyl, the nuclear industry has embraced the concept of safety culture. The work on safety culture has been used to develop programs and concepts in the culture of Material Protection, Control, and Accounting and Nuclear Security Culture. More recently, some work has been done on defining an International Safeguards Culture. Others have spoken about a 3S Culture, but there has been little rigorous consideration of the concept. This paper attempts to address 3S Culture, to begin to evaluate the merit of the concept, and to propose a definition. The paper is followed by the slides of the presentation. (authors)

  15. Vaporization of In2Te3(s)

    The vaporization chemistry of In2Te3(s) was studied by the computerautomated simultaneous Knudsen-effusion and torsion-effusion method, by high-temperature mass spectrometry, and by ancillary methods. The first absolute measurements of the vapor pressure of In2Te3 are reported. In2Te3(s) vaporized incongruently in the temperatue range 701-889 K and produced Te2(g) and a solid-solution, (Xsub(In)=0.42 and Xsub(Te)=0.58). The standard enthalpy of the reaction at 298 K, ΔH0 (298 K) by the third-law method was 136.0 +- 0.3 kJ/mol of vapor. The above solid solution vaporized incongruently and produced in InTe(s) and a vapor which consisted of Te2(g) and In2Te(g). InTe(s) vaporized congruently in the range 701-887 K and produded Te2(g) and In2Te(g); the third-law ΔH0sub(ν) (298 K) was 201.5 +- 1.0 kJ/mol. These results were at variance with the literature on vaporization of In2Te3(s) where both congruent vaporization and incongruent vaporization to give InTe(s) are separately reported. Further, InTe(s) was reported to vaporize incongruently. These differences are discussed. (Author)

  16. P3P semantic checker of site behaviours

    Grande, Robson Eduardo; Zorzo, Sérgio Donizetti

    2006-01-01

    The interactive use of the web between users and service providers introduces a privacy problem that involves the undesired disclosing of user personal information, mainly with the presence of personalization that needs this type of information. Also there are many manners to face it, but the Platform for Privacy Preferences (P3P) is one that provides a variable level of privacy for the user’s browsing. However, the P3P only introduces a privacy contract between the site and the user, without...

  17. Band structure and electron-phonon coupling in H3S : A tight-binding model

    Ortenzi, L.; Cappelluti, E.; Pietronero, L.

    2016-08-01

    We present a robust tight-binding description, based on the Slater-Koster formalism, of the band structure of H3S in the Im3 ¯m structure, stable in the range of pressure P =180 -220 GPa. We show that the interatomic hopping between the 3 s and 3 p orbitals (and partially between the 3 p orbitals themselves) of sulfur is fundamental to capturing the relevant physics associated with the Van Hove singularities close to the Fermi level. Comparing the model so defined with density functional theory calculations we obtain a very good agreement not only of the overall band structure but also of the low-energy states and the Fermi surface properties. The description in terms of Slater-Koster parameters permits us also to evaluate at a microscopic level a hopping-resolved linear electron-lattice coupling which can be employed for further tight-binding analyses also at a local scale.

  18. MAP3S precipitation chemistry network: seventh periodic summary report, 1983. [MAP3S Network

    Rothert, J.E.; Dana, M.T.

    1984-11-01

    This summary report, the seventh in the series, contains complete field and chemical data from the MAP3S Precipitation Chemistry Network for the year 1983. Sections cover QA/QC of the MAP3S/PCN; network history, network site information and a MAP3S/PCN bibliography; and a brief statistical look at the laboratory operations for 1983. There is also a brief statistical summary for 1982 to 1983. Included under the Quality Control section are the QA audits for site performance, laboratory comparisons, field blank and pH test results, and sample shipping and analysis results. Included is a listing of cooperating organizations and personnel for the MAP3S/PCN. 10 references, 10 figures, 32 tables.

  19. A developmental toxicity study of 3S, 3'S-Astaxanthin in New Zealand white rabbits.

    Schneider, Steffen; Mellert, Werner; Schulte, Stefan; van Ravenzwaay, Bennard

    2016-04-01

    Astaxanthin, a naturally occurring pigment used to give the characteristic orange-pink colour to salmonid fish reared in aquaculture, is also marketed as a dietary supplement. Synthetic 3S, 3'S-Astaxanthin was tested for potential harmful effects on the in utero development of New Zealand white rabbits in a study according to international regulatory guidelines. There were two control groups, one being a placebo administration and three dose levels corresponding to 100, 200, and 400 mg of 3S, 3'S-Astaxanthin per kg body weight/day. The group sizes varied from 23 to 27 litters, providing approximately 200 fetuses per group for evaluation of developmental toxicity. There were no significant effects on the health of the does, nor on the size and viability of the litters. Malformations, both external and internal, were rare and occurred in all groups, including controls with no indication of a treatment relationship. Variations were much more common, being found in all litters. However, when examined by type and frequency, no pattern emerged indicating a relationship to administration of the test substance. It is concluded that administration of 3S, 3'S-Astaxanthin in a gelatin/carbohydrate powder formulation throughout pregnancy up to 400 mg/kg body weight/day is without harmful effects on reproduction or fetal development. PMID:26854919

  20. Dsj meson decay in the C3P0 model

    Full text. Fock-Tani is a field theory formalism appropriated for the simultaneous treatment of composite particles and their constituents. The formalism was originally developed for the treatment of problems in atomic physics and it was extended later on to the treatment of problems on hadron physics. In the Fock-Tani formalism one starts with the Fock representation of the system using field operators of elementary constituents which satisfy canonical (anti) commutation relations. Composite-particle field operators are linear combinations of the elementary-particle operators and do not generally satisfy canonical (anti) commutation relations. 'Ideal' field operators acting on an enlarged Fock space are then introduced in close correspondence with the composite ones. Next, a given unitary transformation, which transforms the single composite states into single ideal states, is introduced. Application of the unitary operator on the microscopic Hamiltonian, or on other hermitian operators expressed in terms of the elementary constituent field operators, gives equivalent operators which contain the ideal field operators. The effective Hamiltonian in the new representation has a clear physical interpretation in terms of the processes it describes. Since all field operators in the new representation satisfy canonical (anti)commutation relations, the standard methods of quantum field theory can then be readily applied. For a long time the pair creation models for strong hadronic decays have been formulated. The 3P0 model is typical decay model which considers only OZI-allowed strong decays. The 3P0 model considers a quark-antiquark par creation in the presence of the initial state meson. The quark-antiquark par is created with the vacuum quantum numbers. This model can also be obtained from the non-relativistic limit of the pair creation Hamiltonian. Applying the Fock-Tani transformation to the pair creation Hamiltonian produces the characteristic expansion in powers of

  1. Ionic rotational branching ratios in resonant enhanced multiphoton ionization of NO via the A2Sigma(+)(3s sigma) and D2Sigma(+)(3p sigma) states

    Rudolph, H.; Mckoy, V.; Dixit, S. N.; Huo, W. M.

    1988-01-01

    Results are presented for the rotationally resolved photoelectron spectra resulting from a (2 + 1) one-color resonant enhanced multiphoton ionization (REMPI) of NO via the rotationally clean S21(11.5) and mixed S11(15.5) + R21(15.5) branches of the 0-0 transition in the D-X band. The calculations were done in the fixed-nuclei frozen core approximation. The resulting photoionization spectra, convoluted with a Lorentzian detection function, agree qualitatively with experimental results of Viswanathan et al. (1986) and support their conclusion that the nonspherical nature of the molecular potential creates a substantial l-mixing in the continuum, which in turn leads to the intense Delta N = 0 peak. The rather strong photoelectron energy dependence of the rotational branching ratios of the D 2Sigma(+) S21(11.5) line was investigated and compared to the weak energy dependence of the A 2Sigma(+) R22(21.5) line.

  2. Doubly excited 3P(e) resonant states in Ps(-)

    Ho, Y. K.; Bhatia, A. K.

    1992-01-01

    Doubly excited 3P(e) resonant states in Ps(-) are calculated using a method of complex-coordinate rotation. Resonance parameters (both resonance positions and widths) for doubly excited states associated with the n = 2, 3, 4, 5, and 6 thresholds of positronium atoms are evaluated using elaborate Hylleraas-type functions. In addition to ten Feshbach-type resonances lying below various Ps thresholds, three shape resonances were identified, one each lying above the n = 2, 4, and 6 Ps thresholds. It is further noted that the energy levels for the present 3P(e) states are nearly degenerate with respect to the previously calculated 1P(0) states. Such a symmetric character suggests that the highly and doubly excited Ps(-), similar to its counterpart in H(-), would exhibit rovibrational behaviors analogous to those of XYX triatomic molecules.

  3. Configuration interaction calculations of positron binding to Be(3P )

    The configuration interaction method is applied to investigate the possibility of positron binding to the metastable beryllium (1s22s2p 3P ) state. The largest calculation obtained an estimated energy that was unstable by 0.00014 Hartree with respect to the Ps + Be+(2s) lowest dissociation channel. It is likely that positron binding to parent states with non-zero angular momentum is inhibited by centrifugal barriers

  4. Spatial and electronic structure of the Ni3P surface

    To understand the catalytic effect in the Ni-Ni3P for the growth of carbon nanostructures, the structural and electronic properties of Ni3P surface are calculated from first-principles calculations. The calculated surface energies for the (0 0 1)-Ni4P4-terminated surface, the (0 0 1)-Ni8-terminated surface, and the (1 1 0)-Ni8-terminated surface show that the (0 0 1)-Ni4P4-terminated surface is energetically more stable within the allowed range of the chemical potential of P. Through the analysis of the partial density of states of Ni and P atoms in surface and bulk states, respectively, it is further found that due to the bond contractions of the surface layer, the core-level shifts of P atoms in the (0 0 1)-Ni4P4-terminated surface make P atoms in the Ni3P particles act as a catalyst. Finally, the obtained results of the work function show that the (0 0 1)-Ni4P4-terminated surface has the largest work function when compared with the other two studied surfaces.

  5. Hyperfine Quenching of the 2s2p 3P0 State of Berylliumlike Ions

    Cheng, K T; Chen, M H; Johnson, W R

    2008-03-13

    The hyperfine-induced 2s2p {sup 3}P{sub 0}-2s{sup 2} {sup 1}S{sub 0} transition rate for Be-like {sup 47}Ti{sup 18+} was recently measured in a storage-ring experiment by Schippers et al. [Phys. Rev. Lett. 98, 033001 (2007)]. The measured value of 0.56(3) s{sup -1} is almost 60% larger than the theoretical value of 0.356 s{sup -1} from a multiconfiguration Dirac-Fock calculation by Marques et al. [Phys. Rev. A 47, 929 (1993)]. In this work, we use a large-scale relativistic configuration-interaction method to calculate these hyperfine-induced rates for ions with Z = 6-92. Coherent hyperfine-quenching effects between the 2s2p {sup 1,3}P{sub 1} states are included in a perturbative as well as a radiation damping approach. Contrary to the claims of Marques et al., contributions from the {sup 1}P{sub 1} state are substantial and lead to a hyperfine-induced rate of 0.67 s{sup -1}, in better agreement with, though larger than, the measured value.

  6. The deexcitation of the Ar (3P2, 3p1 and 1P1) states as measured by absorption both in pure argon and in the presence of additives

    The de-excitation of the 3P2, 3p1 and 1P1 states of argon was studied in pure argon between 10 and 200 torr and in Ar + CO and Ar + H2 mixtures. These states are populated after excitation of the gas by a short (20 ns) pulse of 500 keV electrons (FEBETRON). Under our experimental conditions, the relation between the measured optical density of the lines studied and the concentration of absorbing species was found to be: DO = log I0/I ∝ (lC)n with n = 0,4. The three body rate constants k2 were measured for the two resonant states 3p1 (k2 = (1,65 ± 0,3) x 10-32 cm6 s-1) and 1P1 (k2 = (1,0 ± 0,2) x 10-32 cm6 s-1); they had not been considered in previous low pressure studies. For the metastable state 3P2, the measured value of k2 ((1,6 ± 0,3) x 10-32 cm6 s-1) is in good agreement with those found in the literature. However, our two body rate constant k1 is about ten times higher than that found in measurements at low pressure. This difference could be due to a collision-induced emission process at high pressure. The rate constants for the quenching by CO and H2 were measured for the metastable state 3P2 (1,85 and 10,5 x 10-11 cm3 s-1) and for the resonant states 3P1 (4,5 and 20 x 10-11 cm3 s-1) and 1P1 (8,5 and 33 X 10-11 cm3 s-1). Comparison of the de-excitation cross sections of resonant and metastable states should lead to a better understanding of energy transfer processes from these latter. (author)

  7. Einstein A-coefficients for transitions among the 3s23p3 states of S II

    Einstein A-coefficients for transitions among the 3s23p3 states of S II, calculated with the CIV3 code, are found to be up to ∝ 25% different from those of Mendoza and Zeippen. These new results are used to derive the theoretical emission line ratio R = I(3s23p34So3/2-3s2 3p32Do5/2)/I(3s33p34So3/2-3s23p32Do3/2) = I(6717 A)/I(6730 A), which is a very useful electron density diagnostic for gaseous nebulae. The present diagnostics are up to ∝ 10% larger than those deduced using the A-values of Mendoza and Zeippen, and will lead to electron density estimates up to ∝ 50% greater. (orig.)

  8. JS3P: junior staff programme pilot project

    Pretrel, H.; Tregoures, N.; Bessiron, V.; Dehoyos, A.; Delvallee, I.; Brisson, N.; Debayle, C.; Dubreuil, M.; Nicaise, G.; Perignon, J.P.; Richard, J. [Institut de Radioprotection et de Surete Nucleaire (IRSN), 13 - Saint-Paul-lez-Durance (France); Reinke, N.; Kaulard, J.; Burgener, M.; Keesmann, S.; Schramm, B.; Seubert, A.; Sternkopf, J.; Thuma, G.; Weber, S. [Gesellschaft fuer Anlagen- und Reaktorsicherheit mbH (GRS), Koln (Germany); Smidts, O.; Maillet, E.; Bucalossi, A.; Van haesendonck, M.; Uyttenhove, W.; Mertens, J. [AVN, Bruxelles (Belgium)

    2006-07-01

    Concept: The objective of the project is to allow junior staff members from the European Technical Safety Organisations (TSOs), IRSN, GRS and AVN, to work together with the final goal of creating a junior staff network, based on technical, cultural and personal interests. These projects are to show junior staff members at a very early stage during their career the need for European collaborations. They are also a tool to explore new subjects of co-operation. It is an initiative that should strengthen the links between the organisations and contribute to establishing the future of nuclear safety in Europe. A JS3P (Junior Staff Programme Pilot Project) is a project done jointly by 'junior' staff members from the three TSOs, where experience of 'seniors' is also integrated when needed. Compared to other collaborative activities, it has certain specific features. The JS3P favours staff exchanges, and technical meetings of several days should be planned during a project in order to encourage people to work together. Technical objectives are shared and the work is done jointly (reports, articles). The team involved in the JS3P should be as small as possible to favour its efficiency. The JS3P is short and easy to realize. Its duration is fixed to a maximum of about 12 months with the option to be prolonged. Typical topics are bibliographic work, comparison issues, scientific surveys, benchmark exercises and prospective investigations on innovative ideas. They can be linked to existing joint projects and then form a smaller module integrated into the large project. Topics may concern prospective issues, tentatively investigating new topics that can be seen as exploratory co-operation projects. Subjects may also concern research issues that are not a priority but that deserve to be investigated as new attractive topics. The JS3P is defined and managed by junior staff members. It is approved by a management board committee and supervised by a technical

  9. JS3P: junior staff programme pilot project

    Concept: The objective of the project is to allow junior staff members from the European Technical Safety Organisations (TSOs), IRSN, GRS and AVN, to work together with the final goal of creating a junior staff network, based on technical, cultural and personal interests. These projects are to show junior staff members at a very early stage during their career the need for European collaborations. They are also a tool to explore new subjects of co-operation. It is an initiative that should strengthen the links between the organisations and contribute to establishing the future of nuclear safety in Europe. A JS3P (Junior Staff Programme Pilot Project) is a project done jointly by 'junior' staff members from the three TSOs, where experience of 'seniors' is also integrated when needed. Compared to other collaborative activities, it has certain specific features. The JS3P favours staff exchanges, and technical meetings of several days should be planned during a project in order to encourage people to work together. Technical objectives are shared and the work is done jointly (reports, articles). The team involved in the JS3P should be as small as possible to favour its efficiency. The JS3P is short and easy to realize. Its duration is fixed to a maximum of about 12 months with the option to be prolonged. Typical topics are bibliographic work, comparison issues, scientific surveys, benchmark exercises and prospective investigations on innovative ideas. They can be linked to existing joint projects and then form a smaller module integrated into the large project. Topics may concern prospective issues, tentatively investigating new topics that can be seen as exploratory co-operation projects. Subjects may also concern research issues that are not a priority but that deserve to be investigated as new attractive topics. The JS3P is defined and managed by junior staff members. It is approved by a management board committee and supervised by a technical steering committee

  10. Thermodynamic properties of SrMoO3(s) and BaMoO3(s)

    Enthalpy increment measurements for SrMoO3(s) and BaMoO3(s) have been carried out using a high temperature Calvet drop calorimeter. The data were least squares fitted using the constraints that Cpo(298.15 K) values are from literature and Ho(T)-Ho(298.15 K) at 298.15 K equals zero. The enthalpy increment values for SrMoO3(s) and BaMoO3(s) can be given, respectively, by the following equations: Ho(T) - Ho(298.15 K) (J/mol) 123.2 T(K) + 8.092x10-3 T2(K) + 19.998x105/T(K) - 44162 (426 to 1011 K). Ho(T) - Ho(298.15 K)(J/mol) = 132.72 T(K) + 7.3646x10-3 T2 (K) + 27.696x 105/T(K) - 49539 (478 to 1011 K). The first differential of the above equations with respect to temperature gives Cpo(T). Other thermal properties were then derived. (author). 7 refs., 2 tabs

  11. Experimental and theoretical studies of isomeric CH3S2 and CH3S+2

    By combining molecular beam photodissociation and photoionization measurements with ab initio Gaussian-2 (G2) calculations on the CH3S2 and CH3S+2 systems, we have shown that CH3SS is the dominant isomer formed in the photodissociation process, CH3SSCH3+hν(193 nm) →CH3S2+CH3. The experimental ionization energy for CH3SS (8.97±0.02 eV) and the heat of formation at 0 K for CH3SS+ (217.7±1.2 kcal/mol) are in excellent agreement with the G2 results. The photoionization efficiency spectrum observed for CH3SS is also consistent with the theoretical prediction that the Franck--Condon factor for the photoionization process, CH3SS+hν →CH3SS++e-, is not favorable. Based on the statistical modeling of experimental rates obtained previously for HS loss in the unimolecular decomposition of CH3SSCH+3 and the comparison with G2 ab initio predictions, we conclude that CH2SSH+ is most likely the isomer structure formed near the experimental appearance energy (11.07 eV) observed for the photodissociative ionization process, CH3SSCH3+hν→CH3S+2+CH3+e-

  12. Highly charged swelling mica reduces Cu bioavailability in Cu-contaminated soils

    This is the first test of a highly charged swelling mica's (Na-2-mica) ability to reduce the plant-absorbed Cu in Cu-contaminated soils from Chile. Perennial ryegrass (Lolium perenne L.) was grown in two acid soils (Sector 2: pH 4.2, total Cu = 172 mg Cu kg-1 and Sector 3: pH 4.2, total Cu = 112 mg Cu kg-1) amended with 0.5% and 1% (w/w) mica, and 1% (w/w) montmorillonite. At 10 weeks of growth, both mica treatments decreased the shoot Cu of ryegrass grown in Sector 2 producing shoot Cu concentrations above 21-22 mg Cu kg-1 (the phytotoxicity threshold for that species), yet the mica treatments did not reduce shoot Cu concentrations when grown in Sector 3, which were at a typical level. The mica treatments improved shoot growth in Sector 3 by reducing free and extractable Cu to low enough levels where other nutrients could compete for plant absorption and translocation. In addition, the mica treatments improved root growth in both soils, and the 1% mica treatment reduced root Cu in both soils. This swelling mica warrants further testing of its ability to assist re-vegetation and reduce Cu bioavailability in Cu-contaminated surface soils. - In situ remediation of Cu-contaminated soils with a synthetic mica (Na-2-mica) will aid in re-vegetative efforts

  13. Products of the Benzene + O(3P) Reaction

    Taatjes, Craig A.; Osborn, David L.; Selby, Talitha M.; Meloni, Giovanni; Trevitt, Adam J.; Epifanovsky, Evgeny; Krylov, Anna I.; Sirjean, Baptiste; Dames, Enoch; Wang, Hai

    2009-12-21

    The gas-phase reaction of benzene with O(3P) is of considerable interest for modeling of aromatic oxidation, and also because there exist fundamental questions concerning the prominence of intersystem crossing in the reaction. While its overall rate constant has been studied extensively, there are still significant uncertainties in the product distribution. The reaction proceeds mainly through the addition of the O atom to benzene, forming an initial triplet diradical adduct, which can either dissociate to form the phenoxy radical and H atom, or undergo intersystem crossing onto a singlet surface, followed by a multiplicity of internal isomerizations, leading to several possible reaction products. In this work, we examined the product branching ratios of the reaction between benzene and O(3P) over the temperature range of 300 to 1000 K and pressure range of 1 to 10 Torr. The reactions were initiated by pulsed-laser photolysis of NO2 in the presence of benzene and helium buffer in a slow-flow reactor, and reaction products were identified by using the multiplexed chemical kinetics photoionization mass spectrometer operating at the Advanced Light Source (ALS) of Lawrence Berkeley National Laboratory. Phenol and phenoxy radical were detected and quantified. Cyclopentadiene and cyclopentadienyl radical were directly identified for the first time. Finally, ab initio calculations and master equation/RRKM modeling were used to reproduce the experimental branching ratios, yielding pressure-dependent rate expressions for the reaction channels, including phenoxy + H, phenol, cyclopentadiene + CO, which are proposed for kinetic modeling of benzene oxidation.

  14. Photoinduced Kondo effect in CeZn3P3

    Kitagawa, J.; Kitajima, D.; Shimokawa, K.; Takaki, H.

    2016-01-01

    The Kondo effect, which originates from the screening of a localized magnetic moment by a spin-spin interaction, is widely observed in nonartificial magnetic materials, artificial quantum dots, and carbon nanotubes. In devices based on quantum dots or carbon nanotubes that target quantum information applications, the Kondo effect can be tuned by a gate voltage, a magnetic field, or light. However, the manipulation of the Kondo effect in nonartificial materials has not been thoroughly studied; in particular, the artificial creation of the Kondo effect remains unexplored. Per this subject study, however, a route for the optical creation of the Kondo effect in the nonartificial material p -type semiconductor CeZn3P3 is presented. The Kondo effect emerges under visible-light illumination of the material by a continuous-wave laser diode and is ultimately revealed by photoinduced electrical resistivity, which clearly exhibits a logarithmic temperature dependency. By contrast, a La-based compound (LaZn3P3 ) displays only normal metallic behavior under similar illumination. The photoinduced Kondo effect, which occurs at higher temperatures when compared with the Kondo effect in artificial systems, provides a potential range of operation for not only quantum information/computation devices but also for operation of magneto-optic devices, thereby expanding the range of device applications based on the Kondo effect.

  15. Amyloid-β Peptide Aβ3pE-42 Induces Lipid Peroxidation, Membrane Permeabilization, and Calcium Influx in Neurons.

    Gunn, Adam P; Wong, Bruce X; Johanssen, Timothy; Griffith, James C; Masters, Colin L; Bush, Ashley I; Barnham, Kevin J; Duce, James A; Cherny, Robert A

    2016-03-18

    Pyroglutamate-modified amyloid-β (pE-Aβ) is a highly neurotoxic amyloid-β (Aβ) isoform and is enriched in the brains of individuals with Alzheimer disease compared with healthy aged controls. Pyroglutamate formation increases the rate of Aβ oligomerization and alters the interactions of Aβ with Cu(2+) and lipids; however, a link between these properties and the toxicity of pE-Aβ peptides has not been established. We report here that Aβ3pE-42 has an enhanced capacity to cause lipid peroxidation in primary cortical mouse neurons compared with the full-length isoform (Aβ(1-42)). In contrast, Aβ(1-42) caused a significant elevation in cytosolic reactive oxygen species, whereas Aβ3pE-42 did not. We also report that Aβ3pE-42 preferentially associates with neuronal membranes and triggers Ca(2+) influx that can be partially blocked by the N-methyl-d-aspartate receptor antagonist MK-801. Aβ3pE-42 further caused a loss of plasma membrane integrity and remained bound to neurons at significantly higher levels than Aβ(1-42) over extended incubations. Pyroglutamate formation was additionally found to increase the relative efficiency of Aβ-dityrosine oligomer formation mediated by copper-redox cycling. PMID:26697885

  16. Microstructure and Strength of Brazed Joints of Ti3Al Base Alloy with Cu-P Filler Metal

    Peng HE; Jicai FENG; Heng ZHOU

    2005-01-01

    Brazing of Ti3Al alloys with the filler metal Cu-P was carried out at 1173~1273 K for 60~1800 s. When products are brazed, the optimum brazing parameters are as follows: brazing temperature is 1215~1225 K; brazing time is 250~300 s. Four kinds of reaction products were observed during the brazing of Ti3Al alloys with the filler metal Cu-P, i.e., Ti3Al phase with a small quantity of Cu (Ti3Al(Cu)) formed close to the Ti3Al alloy; the TiCu intermetallic compounds layer and the Cu3P intermetallic compounds layer formed between Ti3Al(Cu) and the filler metal, and a Cu-base solid solution formed with the dispersed Cu3P in the middle of the joint. The interfacial structure of brazed Ti3Al alloys joints with the filler metal Cu-P is Ti3Al/Ti3Al(Cu)/TiCu/Cu3P/Cu solid solution (Cu3P)/Cu3P/TiCu/Ti3Al(Cu)/Ti3Al, and this structure will not change with brazing time once it forms. The thickness of TiCu+Cu3P intermetallic compounds increases with brazing time according to a parabolic law. The activation energy Q and the growth velocity K0 of reaction layer TiCu+Cu3P in the brazed joints of Ti3Al alloys with the filler metal Cu-P are 286 k J/mol and 0.0821 m2/s, respectively, and growth formula was y2=0.0821exp(-34421.59/T)t.Careful control of the growth for the reaction layer TiCu+Cu3P can influence the final joint strength. The formation of the intermetallic compounds TiCu+Cu3P results in embrittlement of the joint and poor joint properties. The Cu-P filler metal is not fit for obtaining a high-quality joint of Ti3Al brazed.

  17. Safeguards-by-design: 3S integration

    integration of nuclear safeguards, safety, and security (3S), is a logical and important step in the evolution of the design process, as has been recognized by the IAEA and member states. Integrating SBD with tight links to safety as well takes advantage of the maturity of the nuclear safety experience, properly coordinates the safety requirements with the safeguards and security requirements, and minimizes the negative impact of retrofits during design and construction. (author)

  18. First Detection of [C I] $^3$P$_1$-$^3$P$_0$ Emission from a Protoplanetary Disk

    Tsukagoshi, Takashi; Saito, Masao; Kitamura, Yoshimi; Shimajiri, Yoshito; Kawabe, Ryohei

    2015-01-01

    We performed single point [C I] $^3$P$_1$-$^3$P$_0$ and CO J=4-3 observations toward three T Tauri stars, DM Tau, LkCa 15, and TW Hya, using the Atacama Large Millimeter/submillimeter Array (ALMA) Band 8 qualification model receiver installed on the Atacama Submillimeter Telescope Experiment (ASTE). Two protostars in the Taurus L1551 region, L1551 IRS 5 and HL Tau, were also observed. We successfully detected [C I] emission from the protoplanetary disk around DM Tau as well as the protostellar targets. The spectral profile of the [C I] emission from the protoplanetary disk is marginally single-peaked, suggesting that atomic carbon (C) extends toward the outermost disk. The detected [C I] emission is optically thin and the column densities of C are estimated to be <~10$^{16}$ cm$^{-2}$ and ~10$^{17}$ cm$^{-2}$ for the T Tauri star targets and the protostars, respectively. We found a clear difference in the total mass ratio of C to dust, $M$(C)/$M$(dust), between the T Tauri stars and protostellar targets; t...

  19. Is Upsilon(3S) a pure S-wave?

    Chakravarty, S; Ko, P; Chakravarty, Sumantra; Kim, Sun Myong; Ko, Pyungwon

    1993-01-01

    Assuming the QCD multipole expansion is applicable to hadronic transitions of Upsilon(3S) into lower level bottomonia, we consider the possibility that Upsilon(3S) has a D-wave component. This assumption leads to a natural explanation of the pi-pi spectrum in Upsilon(3S) -> Upsilon(1S) pi-pi. Consequences of this assumption on other hadronic and radiative transitions of Upsilon(3S) are also discussed in the same context.

  20. Untersuchung und Charakterisierung des Phasengebietes M-Q-X (M = Ag, Cu; Q = Chalkogen; X = Halogen)

    Giller, Malte

    2015-01-01

    Diese Dissertation beschreibt die Synthese und Charakterisierung von neuen Verbindungen, im Phasengebiet Cu-Te-Br und Cu-Te-S, sowie der festen Lösung von Cu10Te4Cl3 und Ag10Te4Br3. Hierbei wurden drei neue Phasen, Cu4.8(1)Te3Br, Cu5.4(1)Te3Br und Cu6Te3S isoliert und als kupfergefüllte Varianten des Cr3Si-Strukturtyps charakterisiert.

  1. Rydberg series in the photoionization of the excited 1s2s3s 1,3Se states of atomic beryllium

    Photoionization cross sections for ionization to Be+(2s, 2p, 3s, 3p, and 3d) states from the excited 2s3s 1,3S states of atomic beryllium, which contain several autoionizing Rydberg series of resonances converging to the Be+(2p, 3s, 3p, and 3d) states, have been calculated by an enhanced noniterative eigenchannel R-matrix method. Lower members of the Rydberg series of resonances with n ≤ 10 are identified along with the calculated resonance positions Er, effective quantum numbers n*, and widths Γ. The present results are compared with those of previous calculation and very good agreement between them is noted. There is excellent agreement between length and velocity gauges in the present calculation. (author)

  2. The synthesis of the heterocubane cluster [{CpMn}4(μ3-P)4] as a tetrahedral shaped starting material for the formation of polymeric coordination compounds.

    Heinl, Sebastian; Kiefer, Konrad; Balázs, Gábor; Wickleder, Claudia; Scheer, Manfred

    2015-09-11

    Thermolysis of [CpMn(η(6)-cht)] with P4 in 1,3-diisopropylbenzene leads to the formation of the heterocubane [Cp4Mn4P4] () in high yields, as a rare example of 'naked' phosphorus containing complexes of manganese. Compound is characterized and studied by DFT calculations and reflection measurements. 1D coordination polymers [{(CpMn)4(μ3-P)4}(CuX)]n (2-Cl: X = Cl; 2-Br: X = Br) are obtained in the reaction with CuX. Furthermore, it is shown that all four P atoms in can be addressed for a coordination towards cymantrene resulting in [{(CpMn)4(μ3-P)4}{CpMn(CO)2}n] (: n = 1; : n = 2; : n = 3; : n = 4), and shows that is a tetra-topic building block in coordination chemistry. PMID:26225545

  3. Gibbs energy of formation of UPd3(s)

    Gibbs energy of formation of UPd3(s) has been determined by measuring the equilibrium CO(g) pressure over {UO2(s) + C(s) + UPd3(s) + UPd4(s)} and is given as (ΔfG0m(UPd3,s,T) kJ mol-1±4.1=-526.9+0.1259 T (K), (1175≤T (K)≤1333) Using the required literature data, ΔfH0m(UPd3, s, 298.15 K) has been calculated as -(502.3 ± 5.1) kJ mol-1

  4. Promising bifunctional chelators for copper 64-PET imaging: practical (64)Cu radiolabeling and high in vitro and in vivo complex stability.

    Wu, Ningjie; Kang, Chi Soo; Sin, Inseok; Ren, Siyuan; Liu, Dijie; Ruthengael, Varyanna C; Lewis, Michael R; Chong, Hyun-Soon

    2016-04-01

    Positron emission tomography (PET) using copper-64 is a sensitive and non-invasive imaging technique for diagnosis and staging of cancer. A bifunctional chelator that can present rapid radiolabeling kinetics and high complex stability with (64)Cu is a critical component for targeted PET imaging. Bifunctional chelates 3p-C-NE3TA, 3p-C-NOTA, and 3p-C-DE4TA were evaluated for complexation kinetics and stability with (64)Cu in vitro and in vivo. Hexadentate 3p-C-NOTA and heptadentate 3p-C-NE3TA possess a smaller TACN-based macrocyclic backbone, while nonadentate 3p-C-DE4TA is constructed on a larger CYCLEN-based ring. The frequently explored chelates of (64)Cu, octadentate C-DOTA and hexadentate C-NOTA were also comparatively evaluated. Radiolabeling kinetics of bifunctional chelators with (64)Cu was assessed under mild conditions. All bifunctional chelates instantly bound to (64)Cu in excellent radiolabeling efficiency at room temperature. C-DOTA was less efficient in binding (64)Cu than all other chelates. All (64)Cu-radiolabeled bifunctional chelates remained stable in human serum without any loss of (64)Cu for 2 days. When challenged by an excess amount of EDTA, (64)Cu complexes of C-NOTA, 3p-C-NE3TA and 3p-C-NOTA were shown to be more stable than (64)Cu-C-DOTA and (64)Cu-3p-C-DE4TA. (64)Cu complexes of the new chelates 3p-C-NE3TA and 3p-C-NOTA displayed comparable in vitro and in vivo complex stability to (64)Cu-C-NOTA. In vivo biodistribution result indicates that the (64)Cu-radiolabeled complexes of 3p-C-NOTA and 3p-C-NE3TA possess excellent in vivo complex stability, while (64)Cu-3p-C-DE4TA was dissociated as evidenced by high renal and liver retention in mice. The results of in vitro and in vivo studies suggest that the bifunctional chelates 3p-C-NE3TA and 3p-C-NOTA offer excellent chelation chemistry with (64)Cu for potential PET imaging applications. PMID:26666778

  5. Variation of 3s photoionization resonance structures in a serial atomic number species Ar, K, and Ca

    Subvalence 3s-shell photoionization resonances of Ca were measured with monochromatized synchrotron radiation and photoion time-of-flight spectroscopy method. Charge resolved photoion yield spectra were obtained. Broad peak structures were found in the Ca+ spectrum and shallow window structures were found in the Ca2+ spectrum. We performed MCDF calculations to assign the resonance structures. The 3s-shell photoionization of Ar and K were also measured for comparison. A systematic increase was observed in Fano-Beutler parameter and in the resonance width along with the increase of atomic number from Z=18(Ar) to 20(Ca). We discuss also the spectral structures that could be of the 3p double-shake-up satellites, which are observed in the 3s photoionization region. (author)

  6. Nascent 60S ribosomal subunits enter the free pool bound by Nmd3p.

    Ho, J. H.; Kallstrom, G; Johnson, A. W.

    2000-01-01

    Nmd3p from yeast is required for the export of the large (60S) ribosomal subunit from the nucleus (Ho et al., 2000). Here, we show that Nmd3p forms a stable complex with free 60S subunits. Using an epitope-tagged Nmd3p, we show that free 60S subunits can be coimmunoprecipitated with Nmd3p. The interaction was specific for 60S subunits; 40S subunits were not coimmunoprecipitated. Using this coprecipitation technique and pulse-chase labeling of ribosomal subunit proteins we showed that Nmd3p bo...

  7. Linkage of autosomal dominant dystrophic epidermolysis bullosa in three British families to the marker D3S2 close to the COL7A1 locus.

    al-Imara, L; Richards, A J; Eady, R A; Leigh, I M; Farrall, M; Pope, F M

    1992-01-01

    Linkage of the anonymous marker D3S2 at 3p21 has been shown in three British families with dominant dystrophic epidermolysis bullosa with a combined lod score of 6.75 at theta = 0. This locus is close to the collagen type VII locus implying that abnormalities of this gene cause dominant dystrophic epidermolysis bullosa.

  8. Computational studies of modified [Fe3S4] clusters: Why iron is optimal

    Kepp, Kasper Planeta

    2008-01-01

    This work reports density functional computations of metal-substituted models of biological [Fe3S4] clusters in oxidation states [MFe2S4]+/0/−1 (M = Mn, Fe, Co, Ni, Cu, Zn, and Mo). Geometry optimization with a dielectric screening model is shown to provide a substantial improvement in structure......, compared to earlier used standard procedures. The error for average Fe–S bonds decreased from 0.038 Å to 0.016 Å with this procedure. Four density functionals were compared, B3LYP, BP86, TPSS, and TPSSh. B3LYP and to a lesser extent TPSSh energies were inconsistent with experiment for the oxidized [Fe3S4......]+ cluster. BP86 (and to a slightly lesser extent TPSS) was within expected theoretical and experimental uncertainties for all oxidation states, the only qualitative error being 5 kJ/mol in favor of the MS = 3/2 configuration for the [Fe3S4]+ cluster, so BP86 was used for quantitative results. Computed...

  9. Mn 3s exchange splitting in mixed-valence manganites.

    Galakhov, V. R.; Demeter, M.; Bartkowski, S.; Neumann, M.; Ovechkina, N. A.; Kurmaev, E. Z.; Lobachevskaya, N. I.; Mukovskii, Ya. M.; Mitchell, J.; Ederer, D. L.; Russian Academy of Sciences; Univ. of Osnabruck; Moscow State Steel and Alloys Inst.; Tulane Univ.

    2002-03-15

    We present Mn 3s x-ray photoelectron spectra of manganese oxides with the Mn formal valency from 2+ to 4+. We found that the Sr{sup 2+} doping or cation deficiency in manganites do not change the Mn 3s splitting in manganites with the Mn formal valency from 3.0+ to 3.3+. We suggest that doping holes are localized in O 2p states.

  10. Accurate long-range coefficients for two excited like isotope He atoms: He(2 1P)-He(2 1P), He(2 1P)-He(2 3P), and He(2 3P)-He(2 3P)

    A general formalism is used to express the long-range potential energies in inverse powers of the separation distance between two like atomic or molecular systems with P symmetries. The long-range molecular interaction coefficients are calculated for the molecular symmetries Δ, Π, and Σ, arising from the following interactions: He(2 1P)-He(2 1P), He(2 1P)-He(2 3P), and He(2 3P)-He(2 3P). The electric quadrupole-quadrupole term C5, the van der Waals (dispersion) term C6, and higher-order terms C8 and C10 are calculated ab initio using accurate variational wave functions in Hylleraas coordinates with finite nuclear mass effects. A comparison is made with previously published results where available

  11. Crystal structure of bis{S-hexyl 3-[4-(dimethylaminobenzylidene]dithiocarbazato-κ2N3,S}copper(II

    E. Zangrando

    2015-06-01

    Full Text Available In the title complex, [Cu(C16H24N3S22], the CuII atom is coordinated by two azomethine N and two thiolate S atoms of the chelating Schiff base ligands, resulting in a distorted square-planar coordination environment. The S—Cu—N chelating angle is of 84.41 (5°. The CuII atom is located on a crystallographic inversion centre, leading to a trans configuration of the N,S-chelating ligands.

  12. Thermodynamic properties of SrRuO3(s)

    The enthalpy increment measurements and the standard molar Gibb's energy of formation of SrRuO3(s) were measured using a high-temperature Calvet micro-calorimeter and a galvanic cell, respectively. The enthalpy increments can be represented by the polynomial expression: H0(T)-H0(298.15 K) (J mol-1)=-43517.2+120.8T (K)+0.898x10-2T2 (K)+19.97x105/T (K) [SrRuO3(s), 310.4≤T (K)≤798.8]. The heat capacity C0p,m(T), the first differential of H0(T)-H0(298.15 K) with respect to temperature is given by: C0p,m (SrRuO3, s, T) (J mol-1 K-1)=120.8+1.796x10-2T (K)-19.97x105/T2 (K). The standard Gibbs energy of formation of SrRuO3(s) has been determined by a galvanic cell using CaF2(s) as the solid electrolyte. The fluoride cell is represented by: (-)Pt/O2(g), {CaO(s)+CaF2(s)}//CaF2//{SrF2(s)+RuO2(s)+SrRuO3(s)}, O2(g)/Pt(+). The electromotive force (emf) of the above cell was measured as a function of temperature in the range from 894.4 to 1098 K. The standard Gibb's energy of formation of SrRuO3(s) from elements in their standard state obtained by the fluoride cell can be given by: ΔfG0[SrRuO3(s)]/kJ mol-1(±2)=-941.0+0.2586·(T/K) (894.4av=996.2 K. The heat capacity of SrRuO3(s) determined by Calvet calorimeter and the data obtained from fluoride cell were used to calculate the standard enthalpy and entropy of formation of the compound at 298.15 K. The second law method gives ΔfH0[SrRuO3(s), 298.15 K] and ΔfS0[SrRuO3(s), 298.15 K] of the compound from elements in their standard state to be -955.0 kJ mol-1 and 111.04 J K-1 mol-1, respectively

  13. Synthesis of (3S,4R)-bengamide E

    Qi Jun Liu; Hong Li; Shao Peng Chen; Guo Chun Zhou

    2011-01-01

    (3S,4R)-Bengamide E (2) was synthesized starting from D-glucono-δ-lactone (3) and the key deoxygenation step from 13 to 15 was achieved by the application of NaBH3CN and ZnI2. Compared with natural bengamide E (1), the synthetic compound (3S,4R)-bengamide E (2) was inactive against the cell growth of HUVEC and cancer cells. These data represent the significance of the stereochemistry at C-3 and C-4 of bengamides for structural recognition and binding with the target(s).

  14. The direct measurement of the 3 3P0-3 3P1 fine-structure interval and the gJ-factor of atomic silicon by laser magnetic resonance

    Evenson, K. M.; Beltran-Lopez, V.; Ley-Koo, E.; Inguscio, M.

    1984-01-01

    The J - 1 fine structure interval and the g-factor of the 3P1 state have been determined with high precision in the present laser magnetic resonance measurements of the ground 3p2 3P multiplet of atomic Si. Delta-E(3P1-3P0) = 2,311,755.6(7) MHz, and gJ(3P1) = 1.500830(70). Single-configuration calculations of gJ for 3P1 and 3P2 yield a value for the latter which, at 1.501095, is noted to differ by an unexpectedly large margin from the experimental value.

  15. The effect of Sm, Eu and Yb on the thermoelectric properties of Th/sub 3/P/sub 4/ - type lanthanum sulfide

    The Th/sub 3/P/sub 4/-type lanthanum sulfides are n-type semiconductors and a continuous series of solid solutions is found between the compositions of La/sub 3/S/sub 4/ and La/sub 2/S/sub 3/. These materials are attractive for use in high temperature thermoelectric applications because of their high melting points, low thermal conductivities and their inherent ability to vary the electron concentration from a maximum of 6.02 X 10/sup 21/ cm/sup -3/ for La/sub 3/S/sub 4/ to zero for La/sub 2/S/sub 3/ (i.e., self-doping). In this study, La/sub 3/S/sub 4/ compounds in which trivalent La has been partially substituted by divalent Sm, Eu or Yb (La/sub 3-x/M/sub x/S/sub 4/, x = 0.1 to 0.9) have been prepared by the pressure assisted reaction sintering method and were found to have the Th/sub 3/P/sub 4/ structure. The thermoelectric properties (Seebeck coefficient and electrical resistivity) were measured as a function of temperature and the optimum composition was found for x between 0.2 and 0.3 in which the electrical power factor was a maximum at 10000C

  16. Relativistic effects on the hyperfine structures of 2p4(3P)3p 2Do, 4Do and 4Po in 19F I

    Carette, Thomas; Nemouchi, Messaoud; Li, Jiguang; Godefroid, Michel

    2013-01-01

    The hyperfine interaction constants of the 2p4(3P)3p 2Do_{3/2,5/2}, 4Do_{1/2-7/2} and 4Po_{1/2-5/2} levels in neutral fluorine are investigated theoretically. Large-scale calculations are carried out using the multiconfiguration Hartree-Fock (MCHF) and Dirac-Hartree-Fock (MCDHF) methods. In the framework of the MCHF approach, the relativistic effects are taken into account in the Breit-Pauli approximation using non relativistic orbitals. In the fully relativistic approach, the orbitals are op...

  17. Medium Effects in Cooling of Neutron Stars and $3P_2$ Neutron Gap

    Grigorian, H.; Voskresensky, D.N.(National Research Nuclear University (MEPhI), Moscow, 115409, Russia)

    2005-01-01

    We study the dependence of the cooling of isolated neutron stars on the magnitude of the $3P_2$ neutron gap. It is demonstrated that our ``nuclear medium cooling'' scenario is in favor of a suppressed value of the $3P_2$ neutron gap.

  18. A case of 3p deletion syndrome associated with cerebellar hemangioblastoma.

    Suzuki-Muromoto, Sato; Hino-Fukuyo, Naomi; Haginoya, Kazuhiro; Kikuchi, Atsuo; Sato, Hiroki; Sato, Yuko; Nakayama, Tojo; Kubota, Yuki; Kakisaka, Yosuke; Uematsu, Mitsugu; Kumabe, Toshihiro; Md, Shigeo Kure

    2016-02-01

    We described clinical course of a 24-year-old woman with 3p deletion syndrome associated with cerebellar hemangioblastoma at the age of 16 years old. She presented dysmorphic facial features, growth retardation and severe psychomotor retardation associated with 3p deletion syndrome. We identified de novo 3p deletion encompassing p25 by using array-based comparative genomic hybridization, where causative gene of von Hippel-Lindau (VHL) disease located. Surgical therapy for cerebellar hemangioblastoma was performed, and histological examination was consistent in cerebellar hemangioblastoma. She showed no other tumors associated VHL disease till 24 years old. This is the first case report of a patient with 3p deletion syndrome whose cerebellar hemangioblastoma may be associated with VHL disease. Repeat imaging studies were recommended for the patients with 3p deletion syndrome. PMID:26365017

  19. On the magnetocrystalline anisotropy of greigite (Fe3S 4)

    Winklhofer, M.; Chang, L.; Eder, S.H.K.

    2014-01-01

    The ferrimagnetic mineral greigite (cubic Fe3S4) is well known as an intracellular biomineralization product in magnetic bacteria and as a widely occurring authigenic mineral in anoxic sediments. Due to the lack of suitable single-crystal specimens, the magnetic anisotropy parameters of greigite hav

  20. Towards a Mg lattice clock: Observation of the $^1S_{0}-$$^3P_{0}$ transition and determination of the magic wavelength

    Kulosa, A P; Zipfel, K H; Rühmann, S; Sauer, S; Jha, N; Gibble, K; Ertmer, W; Rasel, E M; Safronova, M S; Safronova, U I; Porsev, S G

    2015-01-01

    We optically excite the electronic state $3s3p~^3P_{0}$ in $^{24}$Mg atoms, laser-cooled and trapped in a magic-wavelength lattice. An applied magnetic field enhances the coupling of the light to the otherwise strictly forbidden transition. We determine the magic wavelength, the quadratic magnetic Zeeman shift and the transition frequency to be 468.463(207)$\\,$nm, -206.6(2.0)$\\,$MHz/T$^2$ and 655 058 646 691(101)$\\,$kHz, respectively. These are compared with theoretical predictions and results from complementary experiments. We also developed a high-precision relativistic structure model for magnesium, give an improved theoretical value for the blackbody radiation shift and discuss a clock based on bosonic magnesium.

  1. Synthetic smythite and monoclinic Fe3S4

    Fleet, Michael E.

    1982-11-01

    Smythite and monoclinic Fe3S4 have been identified by X-ray diffraction procedures in quenched ironsulfide compositions. Both phases appear to be metastable under the conditions of the experiments and their development is structurally induced. Smythite occurs as a coherent twinned intergrowth with hexagonal 3C pyrrhotite. Individual single crystals contain about 50% smythite. Reciprocal lattice rows with h-k ≠ 3n show continuous diffraction streaks. The available data suggest that smythite forms via a “polytypic” displacive transformation, by the introduction of stacking faults in the hexagonal close-packed layers of S atoms in high-temperature 1C pyrrhotite. This is analogous to the transformation of 2H wurtzite to intermediate ordered and disordered ZnS layer sequences. The ideal formula of smythite appears to be Fe13S16. Monoclinic Fe3S4 ( a=5.93, b=3.42, c=10.64 Å, β=91.9°) is present in amounts up to 25% of total sulfides. It has a derivative NiAs-type structure, and is isomorphous with monoclinic Cr3S4 and Fe3Se4. It occurs as small lenticular lamellae within grains of 3C pyrrhotite, and apparently corresponds to the unidentified lamellar phase of Arnold (1962). The lamellae have a rhombohedral morphology, with a habit plane close to {1011}. In single crystal grains of pyrrhotite, monoclinic Fe3S4 in twinned in a manner consistent with transformation from high-temperature 1C pyrrhotite. Although Fe3S4 lamellae have the general appearance of plate martensite, they do not represent a diffusionless transformation.

  2. Ge 3P 6Si 2O 25: A cage structure closely related to the intersecting tunnel structure KMo 3P 6Si 2O 25

    Leclaire, A.; Raveau, B.

    1988-08-01

    A germanosilicophosphate Ge 3P 6Si 2O 25 has been isolated. Its structure was solved from a single-crystal study in the space group P overline31c . Its cell parameters are a = b = 7.994(1) Å, c = 16.513(2) Å, Z = 2. The refinement by full-matrix least-squares calculations leads to R = 0.043 with 686 independent reflections. The structure of this oxide is built up from corner-sharing PO 4 and SiO 4 tetrahedra and GeO 6 octahedra. One observes a feature common to several silicophosphates: the presence of the structural unit P 6Si 2O 25 built up from a disilicate group sharing its corners with six PO 4 tetrahedra. The structural relationships between this oxide and the silicophosphates AMo 3P 6Si 2O 25 and Si 3P 6Si 2O 25 (or Ge 3P 6 Ge 2O 25) are described.

  3. Preparation, spectroscopic investigation and antiproliferative capacity of new metal complexes of (3E)-2-(hydroxyimino)-N-P-Tolyl-3-(P-tolylimino) butanamide

    El-Tabl, Abdou Saad; Abd El-wahed, Moshira Mohamed; Abd El-Razek, Samar Ebrahim

    2013-03-01

    Cr(III), Mn(II), Fe(III), Co(II), Ni(II), Cu(II), Zn(II), Cd(II), Sr(II), Hg(II), Tl(I), UO2(II) and ZrO(II) complexes of (3E)-2-(hydroxyimino)-N-P-Tolyl-3-(P-tolylimino) butanamide have been prepared and characterized by elemental analyses, IR, UV-Vis spectra, magnetic moments, conductances, 1H NMR and mass spectra (ligand and its Zn(II) complex), thermal analyses (DTA and TGA) and ESR measurements. The IR data show that, the ligand behaves as monobasic bidentate or neutral bidentate. Molar conductances in DMF indicate that, the complexes are non-electrolytes. ESR spectra of solid Cu(II) complexes at room temperature show axial type (dx2-y2) with covalent bond character in an octahedral environment. Complexes showed inhibitory activity against hepatocellular carcinoma (HepG-2 cell line).

  4. Electronic and Rovibrational Quantum Chemical Analysis of C$_3$P$^-$: The Next Interstellar Anion?

    Fortenberry, Ryan C

    2015-01-01

    C$_3$P$^-$ is analogous to the known interstellar anion C$_3$N$^-$ with phosphorus replacing the nitrogen in a simple step down the periodic table. In this work, it is shown that C$_3$P$^-$ is likely to possess a dipole-bound excited state. It has been hypothesized and observationally supported that dipole-bound excited states are an avenue through which anions could be formed in the interstellar medium. Additionally, C$_3$P$^-$ has a valence excited state that may lead to further stabilization of this molecule, and C$_3$P$^-$ has a larger dipole moment than neutral C$_3$P ($\\sim 6$ D vs. $\\sim 4$ D). As such, C$_3$P$^-$ is probably a more detectable astromolecule than even its corresponding neutral radical. Highly-accurate quantum chemical quartic force fields are also applied to C$_3$P$^-$ and its singly $^{13}$C substituted isotopologues in order to provide structures, vibrational frequencies, and spectroscopic constants that may aid in its detection.

  5. Electronic and rovibrational quantum chemical analysis of C3P-: the next interstellar anion?

    Fortenberry, Ryan C.; Lukemire, Joseph A.

    2015-11-01

    C3P- is analogous to the known interstellar anion C3N- with phosphorus replacing nitrogen in a simple step down the periodic table. In this work, it is shown that C3P- is likely to possess a dipole-bound excited state. It has been hypothesized and observationally supported that dipole-bound excited states are an avenue through which anions could be formed in the interstellar medium. Additionally, C3P- has a valence excited state that may lead to further stabilization of this molecule, and C3P- has a larger dipole moment than neutral C3P (˜6 D versus ˜4 D). As such, C3P- is probably a more detectable astromolecule than even its corresponding neutral radical. Highly accurate quantum chemical quartic force fields are also applied to C3P- and its singly 13C substituted isotopologues in order to provide structures, vibrational frequencies, and spectroscopic constants that may aid in its detection.

  6. Progress on the Multiphysics Capabilities of the Parallel Electromagnetic ACE3P Simulation Suite

    Kononenko, Oleksiy [SLAC National Accelerator Lab., Menlo Park, CA (United States)

    2015-03-26

    ACE3P is a 3D parallel simulation suite that is being developed at SLAC National Accelerator Laboratory. Effectively utilizing supercomputer resources, ACE3P has become a key tool for the coupled electromagnetic, thermal and mechanical research and design of particle accelerators. Based on the existing finite-element infrastructure, a massively parallel eigensolver is developed for modal analysis of mechanical structures. It complements a set of the multiphysics tools in ACE3P and, in particular, can be used for the comprehensive study of microphonics in accelerating cavities ensuring the operational reliability of a particle accelerator.

  7. Sizeable beta-strength in {sup 31}Ar (β3p) decay

    Koldste, G.T. [Department of Physics and Astronomy, Aarhus University, DK-8000 Aarhus C (Denmark); Blank, B. [Centre d' Études Nucléaire de Bordeaux-Gradignan, CNRS/IN2P3 – Université Bordeaux I, F-33175 Gradignan Cedex (France); Borge, M.J.G.; Briz, J.A.; Carmona-Gallardo, M. [Instituto de Estructura de la Materia, CSIC, E-28006 Madrid (Spain); Fraile, L.M. [Grupo de Física Nuclear, Universidad Complutense, CEI Moncloa, E-28040 Madrid (Spain); Fynbo, H.O.U. [Department of Physics and Astronomy, Aarhus University, DK-8000 Aarhus C (Denmark); Giovinazzo, J. [Centre d' Études Nucléaire de Bordeaux-Gradignan, CNRS/IN2P3 – Université Bordeaux I, F-33175 Gradignan Cedex (France); Johansen, J.G. [Department of Physics and Astronomy, Aarhus University, DK-8000 Aarhus C (Denmark); Jokinen, A. [Department of Physics, University of Jyväskylä, FIN-40351 Jyväskylä (Finland); Jonson, B. [Fundamental Fysik, Chalmers Tekniska Högskola, S-41296 Göteborg (Sweden); Kurturkian-Nieto, T. [Centre d' Études Nucléaire de Bordeaux-Gradignan, CNRS/IN2P3 – Université Bordeaux I, F-33175 Gradignan Cedex (France); Nilsson, T. [Fundamental Fysik, Chalmers Tekniska Högskola, S-41296 Göteborg (Sweden); Perea, A.; Pesudo, V. [Instituto de Estructura de la Materia, CSIC, E-28006 Madrid (Spain); and others

    2014-10-07

    We present for the first time precise spectroscopic information on the recently discovered decay mode β-delayed 3p-emission. The detection of the 3p events gives an increased sensitivity to the high energy part of the Gamow–Teller strength distribution from the decay of {sup 31}Ar revealing that as much as 30% of the strength resides in the β3p-decay mode. A simplified description of how the main decay modes evolve as the excitation energy increases in {sup 31}Cl is provided.

  8. Sizeable beta-strength in 31Ar (beta 3p) decay

    T. Koldste, G.; Blank, B.; J. G. Borge, M.;

    2014-01-01

    We present for the first time precise spectroscopic information on the recently discovered decay mode beta-delayed 3p-emission. The detection of the 3p events gives an increased sensitivity to the high energy part of the Gamow-Teller strength distribution from the decay of 31Ar revealing that as...... much as 30% of the strength resides in the beta-3p decay mode. A simplified description of how the main decay modes evolve as the excitation energy increases in 31Cl is provided....

  9. Investigation of the H-Cu and Cu-Cu bonds in hydrogenated Cu

    Shuttleworth, I. G.

    2013-01-01

    The pure and hydrogenated copper system CuHn (n=0, 0.25, 0.50, 0.75 and 1) has been investigated using LCAO-DFT. The average H-Cu (Cu-Cu) bonding interaction increases (decreases) with n whilst concurrent orbital-resolved studies of the H-Cu interactions showed that the (non-)directional H-Cu bonds become more (less) bonding. This preference for directional bonds is reflected in the Cu-Cu interactions. CuH0.25 is shown to have an unusually localized electronic structure compared to the more hydrogenated systems, and the origins of this structure are discussed.

  10. Inclusive χ(2P) production in Υ(3S) decay

    Using the CsI calorimeter of the CLEO II detector, the spin triplet χb(2P) states are observed in Υ(3S) radiative decays with much higher statistics than seen in previous experiments. The observed mass splittings are not described well by theoretical models, while the relative branching ratios agree with predictions that include relativistic corrections to the radiative transition rates

  11. Fundamental magnetic properties of Greigite (Fe3S4)

    Chang, Liao

    2009-01-01

    Over the last twenty years, greigite (Fe3S4), an authigenic magnetic iron sulphide mineral, has been increasingly identified in sulphate-reducing marine and lacustrine sedimentary systems. Its presence can significantly affect palaeomagnetic and environmental magnetic records. Understanding the recording characteristics of any magnetic mineral requires that its fundamental magnetic properties are known. However, unlike magnetite (Fe3O4) and other common terrestrial magnetic minerals, the fund...

  12. Safeguards-by-Design: An Element of 3S Integration

    In 2008, the '20/20 Vision for the Future' background report by the IAEA Director General identified the possibility of integrating certain activities related to safeguards, safety, and security. Later in the year, the independent Commission report prepared at the request of the IAEA Director General noted that the Agency's's roles in nuclear safeguards, safety, and security (3S) complement and can mutually reinforce each other. Safeguards-by-design (SBD) is a practical measure that strengthens 3S integration, especially for the stage of nuclear facility design and construction, but also with ramifications for other stages of the facility life-cycle. This paper describes the SBD concept, with examples for diverse regulatory environments, being developed in the U.S under the U.S. Department of Energy (DOE) Next Generation Safeguards Initiative and the Advanced Fuel Cycle Initiative. This is compared with related international SBD work performed in the recent IAEA workshop on 'Facility Design and Plant Operation Features that Facilitate the Implementation of IAEA Safeguards'. Potential future directions for further development of SBD and its integration within 3S are identified.

  13. Multiscale Hy3S: Hybrid stochastic simulation for supercomputers

    Kaznessis Yiannis N

    2006-02-01

    Full Text Available Abstract Background Stochastic simulation has become a useful tool to both study natural biological systems and design new synthetic ones. By capturing the intrinsic molecular fluctuations of "small" systems, these simulations produce a more accurate picture of single cell dynamics, including interesting phenomena missed by deterministic methods, such as noise-induced oscillations and transitions between stable states. However, the computational cost of the original stochastic simulation algorithm can be high, motivating the use of hybrid stochastic methods. Hybrid stochastic methods partition the system into multiple subsets and describe each subset as a different representation, such as a jump Markov, Poisson, continuous Markov, or deterministic process. By applying valid approximations and self-consistently merging disparate descriptions, a method can be considerably faster, while retaining accuracy. In this paper, we describe Hy3S, a collection of multiscale simulation programs. Results Building on our previous work on developing novel hybrid stochastic algorithms, we have created the Hy3S software package to enable scientists and engineers to both study and design extremely large well-mixed biological systems with many thousands of reactions and chemical species. We have added adaptive stochastic numerical integrators to permit the robust simulation of dynamically stiff biological systems. In addition, Hy3S has many useful features, including embarrassingly parallelized simulations with MPI; special discrete events, such as transcriptional and translation elongation and cell division; mid-simulation perturbations in both the number of molecules of species and reaction kinetic parameters; combinatorial variation of both initial conditions and kinetic parameters to enable sensitivity analysis; use of NetCDF optimized binary format to quickly read and write large datasets; and a simple graphical user interface, written in Matlab, to help users

  14. miR-1207-3p Is a Novel Prognostic Biomarker of Prostate Cancer.

    Das, Dibash K; Osborne, Joseph R; Lin, Hui-Yi; Park, Jong Y; Ogunwobi, Olorunseun O

    2016-06-01

    MicroRNAs (miRNAs) have been found to be dysregulated in prostate cancer (PCa). In this study, we investigated if miR-1207-3p is capable of distinguishing between indolent and aggressive PCa and if it contributes to explaining the disproportionate aggressiveness of PCa in men of African ancestry (moAA). A total of 404 patients with primary adenocarcinoma of the prostate were recruited between 1988 and 2003 at the Moffitt Cancer Center, Tampa, FL, USA. Patient clinicopathological features and demographic characteristics such as race were identified. RNA samples from 404 postprostatectomy prostate tumor tissue samples were analyzed by real-time quantitative reverse transcription polymerase chain reaction for the mRNA expression of miR-1207-3p. miR-1207-3p expression in PCa that resulted in overall death or PCa-specific death is significantly higher than in PCa cases that did not. The same positive correlation holds true for other clinical characteristics such as biochemical recurrence, Gleason score, clinical stage, and prostate-specific antigen level. Furthermore, miR-1207-3p expression was significantly less in moAA in comparison to Caucasian men. We also evaluated whether miR-1207-3p is associated with clinical outcomes adjusted for age at diagnosis and tumor stage in the modeling. Using competing risk regression, the PCa patients with a high miR-1207-3p expression (≥6 vs 3) had a high risk to develop PCa recurrence (hazard rate = 2.5, P < .001) adjusting for age at diagnosis and tumor stage. In conclusion, miR-1207-3p is a promising novel prognostic biomarker for PCa. Furthermore, miR-1207-3p may also be important in explaining the disproportionate aggressiveness of PCa in moAA. PMID:27267842

  15. MPI spectroscopy in the region of the 3p Rydberg state of some cycloketones

    Kosmidis, C.; Boulakis, G.; Bolovinos, A.; Tsekeris, P.; Brint, P.

    1992-03-01

    The two-photon resonance three photon ionization spectra of cyclopentanone, cyclohexanone and cycloheptanone in the region of the 3p Rydberg state have been recorded, analysed and compared with the one-photon absorption spectra. A new 3p origin is identified for cyclopentanone. The absence from the MPI spectra of a sharp spectral feature that is observed in the absorption spectra is discussed. Photochemical generation of acetaldehyde is observed at high laser intensities and possible mechanisms for this are considered.

  16. Determination of diffusion, reflection and deexcitation coefficients of metastable excited Ne(3P2) atom

    Suzuki, S.; Itoh, H.

    2016-05-01

    The diffusion coefficient of the metastable excited Ne(3P2) atom in neon, the reflection coefficient of Ne(3P2) at the surface of an electrode and the rate coefficient of Ne(3P2) for collisional quenching by Ne(1S0) were determined from the gas pressure dependence of the effective lifetime of Ne(3P2). The effective lifetime of Ne(3P2) was measured from the transient current after turning off the Ultraviolet (UV) light in a Townsend discharge. The observed transient current waveform was analysed by solving the diffusion equation for the metastable excited Ne(3P2) atom using the third kind of boundary condition. The rate coefficient of Ne(3P2) for collisional quenching by Ne(1S0) and the reflection coefficient were determined by a nonspectroscopic method for the first time in neon to the best of our knowledge and were (3.2  ±  0.4)  ×  10‑16 cm3 s‑1 and 0.10  ±  0.04, respectively. The obtained diffusion coefficient at 1 Torr was 177  ±  17 cm2 s‑1, which is consistent with the value reported by Dixon and Grant. Moreover, the present results are compared with the results of Phelps and were found to be in good agreement. We also discuss the deexcitation rate of Ne(3P2) at pressures of up to 60 Torr in comparison with previously reported values.

  17. MiR-373-3p Promotes Invasion and Metastasis of Lung Adenocarcinoma Cells

    Aibing WU

    2015-07-01

    Full Text Available Background and objective Lung cancer is the leading cause of cancer-related deaths worldwide, and metastasis is the major cause of death in lung cancer patients. MiR-373 is closely associated with invasion and metastasis in other tumor cells. This study explored the expression of miR-373-3p in non-small cell lung cancer (NSCLC and its effect on the invasive and metastatic capabilities of lung adenocarcinoma cells, as well as their mechanisms of action. Methods The expression of miR-373-3p in NSCLC tissues and lung adenocarcinoma cell lines was detected by quantitative reverse transcription polymerase chain reaction. The roles of miR-373-3p in regulating lung adenocarcinoma cell invasion and metastatic properties were analyzed with miR-373-3p mimic/inhibitor-transfected cells via Transwell chamber assay. Matrix metalloproteinase MMP-9 and MMP-14 protein levels were detected by Western blot in lung cancer cells after transfection. Results MiR-373-3p was upregulated in 51 NSCLC tissues and 5 NSCLC cell lines. Gain-of-function and loss-of-function studies showed that overexpression of miR-373-3p promoted H1299 cell migration and invasion, which resulted in upregulation of MMP-9 and MMP-14. By contrast, miR-373-3p knockdown inhibited these processes in A549 cells and downregulated the expression of MMP-9 and MMP-14. Conclusion Our results demonstrated that miR-373-3p participated in the invasion and metastasis of lung adenocarcinoma cells, partly by upregulation of MMP-9 and MMP-14.

  18. Ab-initio calculation of the 2s21S0-2s3p 3P1 intercombination transition in beryllium-like ions

    Transition probabilities of the 2s21S0-2s3p 1,3P1 intercombination and resonance lines have been calculated for 14 beryllium-like ions in the atomic range 7 ≤ Z ≤ 36. We used multiconfiguration Dirac-Fock wave functions to explore the effects of configuration interaction, of electron rearrangement as well as of relativity in a consistent scheme along the isoelectronic sequence. To show the number of configurations needed in a proper expansion of the wave functions we systematically enlarged the basis from small to large-scale. For the low-Z elements, virtual excitations of the 2s and 3p electrons up to the 5l subshells contribute significantly to the intercombination probability even though the transition energies remain almost unaffected by excitations beyond the 3l shells. The incomplete orthogonality of the orbital functions due to the rearrangement of the electron density clearly shifts the intercombination rates and appears to be independent of the configuration expansion. This effect decreases, as expected, at higher nuclear charges. (orig.)

  19. miR-193a-3p is a potential tumor suppressor in malignant pleural mesothelioma.

    Williams, Marissa; Kirschner, Michaela B; Cheng, Yuen Yee; Hanh, Jacky; Weiss, Jocelyn; Mugridge, Nancy; Wright, Casey M; Linton, Anthony; Kao, Steven C; Edelman, J James B; Vallely, Michael P; McCaughan, Brian C; Cooper, Wendy; Klebe, Sonja; Lin, Ruby C Y; Brahmbhatt, Himanshu; MacDiarmid, Jennifer; van Zandwijk, Nico; Reid, Glen

    2015-09-15

    Malignant pleural mesothelioma (MPM) is an asbestos-induced cancer with poor prognosis that displays characteristic alterations in microRNA expression. Recently it was reported that the expression of a subset of microRNAs can distinguish between MPM and adenocarcinoma of the lung. However, the functional importance of these changes has yet to be investigated. We compared expression of miR-192, miR-193a-3p and the miR-200 family in normal pleura and MPM tumor specimens and found a statistically significant reduction in the levels of miR-193a-3p (3.1-fold) and miR-192 (2.8-fold) in MPM. Transfection of MPM cells with a miR-193a-3p mimic resulted in inhibition of growth and an induction of apoptosis and necrosis in vitro. The growth inhibitory effects of miR-193a-3p were associated with a decrease in MCL1 expression and were recapitulated by RNAi-mediated MCL1 silencing. Targeted delivery of miR-193a-3p mimic using EDV minicells inhibited MPM xenograft tumour growth, and was associated with increased apoptosis. In conclusion, miR-193a-3p appears to have importance in the biology of MPM and may represent a target for therapeutic intervention. PMID:26125439

  20. Protective role of miR-23b-3p in kainic acid-induced seizure.

    Zhan, Lianbo; Yao, Yi; Fu, Huajun; Li, Zhenghui; Wang, Fengpeng; Zhang, Xiaobin; He, Wencan; Zheng, Weihong; Zhang, Yunwu; Zheng, Honghua

    2016-07-01

    Dysregulation of microRNAs has been proposed to contribute toward epilepsy. The miRNA miR-23b-3p has been found to protect against neuronal apoptosis and the production of reactive oxygen species. In this study, we assessed the potential role of miR-23b-3p in the kainic acid (KA)-induced seizure model. We found that miR-23b-3p levels were significantly decreased in the brain cortex of mice and in cultured mouse primary neurons treated with KA. Importantly, supplement of miR-23b-3p agomir by an intacerebroventricular injection alleviated seizure behaviors and abnormal cortical electroencephalogram recordings in KA-treated mice. Together, these results indicate that miR-23b-3p plays a crucial role in suppressing seizure formation in experimental models of epilepsy and that miR-23b-3p supplement may be a potential anabolic strategy for ameliorating seizure. PMID:27232518

  1. Bonding and electronic properties of the Cu2ZnSnS4 /WZ–ZnO interface from first-principles calculations

    Cheng, Yu-Wen; Tang, Fu-Ling; Xue, Hong-Tao; Liu, Hong-Xia; Gao, Bo; Feng, Yu-Dong

    2016-07-01

    We theoretically explored the interface structure, binding energy, band offsets and electronic properties of the CZTS (1 0 2)/WZ–ZnO (1 1 0) interface from first-principles calculations. The interface has a small lattice mismatch of less than 3.2%. The interface binding energy is about  ‑0.21 J m‑2. The values of band offset indicate that such an interface belongs to the type-I heterojunction. New electronic density of states, the so called interface states, appear near the Fermi level. These states are attributed to Cu 3d, Sn 5s, S 3s and 3p orbitals on the first CZTS layer, Zn 4s and 3d, O 2s and 2p orbitals on the first WZ–ZnO layer. The orbital hybridizations and charge transfers on both sides strengthen the interfacial adhesion.

  2. Increased miR-132-3p expression is associated with chronic neuropathic pain.

    Leinders, M; Üçeyler, N; Pritchard, R A; Sommer, C; Sorkin, L S

    2016-09-01

    Alterations in the neuro-immune balance play a major role in the pathophysiology of chronic neuropathic pain. MicroRNAs (miRNA) can regulate both immune and neuronal processes and may function as master switches in chronic pain development and maintenance. We set out to analyze the role of miR-132-3p, first in patients with peripheral neuropathies and second in an animal model of neuropathic pain. We initially determined miR-132-3p expression by measuring its levels in white blood cells (WBC) of 30 patients and 30 healthy controls and next in sural nerve biopsies of 81 patients with painful or painless inflammatory or non-inflammatory neuropathies based on clinical diagnosis. We found a 2.6 fold increase in miR-132-3p expression in WBC of neuropathy patients compared to healthy controls (panimal model of neuropathic pain, the spared nerve injury model (SNI). For this purpose miR-132-3p expression levels were measured in dorsal root ganglia and spinal cord of rats. Subsequently, miR-132-3p expression was pharmacologically modulated with miRNA antagonists or mimetics, and evoked pain and pain aversion were assessed. Spinal miR-132-3p levels were highest 10days after SNI, a time when persistent allodynia was established (pbehavior in the place escape avoidance paradigm (pbehavior in naïve rats (p<0.001). Taken together these results indicate a pro-nociceptive effect of miR-132-3p in chronic neuropathic pain. PMID:27349406

  3. Misregulation of Scm3p/HJURP causes chromosome instability in Saccharomyces cerevisiae and human cells.

    Prashant K Mishra

    2011-09-01

    Full Text Available The kinetochore (centromeric DNA and associated proteins is a key determinant for high fidelity chromosome transmission. Evolutionarily conserved Scm3p is an essential component of centromeric chromatin and is required for assembly and function of kinetochores in humans, fission yeast, and budding yeast. Overexpression of HJURP, the mammalian homolog of budding yeast Scm3p, has been observed in lung and breast cancers and is associated with poor prognosis; however, the physiological relevance of these observations is not well understood. We overexpressed SCM3 and HJURP in Saccharomyces cerevisiae and HJURP in human cells and defined domains within Scm3p that mediate its chromosome loss phenotype. Our results showed that the overexpression of SCM3 (GALSCM3 or HJURP (GALHJURP caused chromosome loss in a wild-type yeast strain, and overexpression of HJURP led to mitotic defects in human cells. GALSCM3 resulted in reduced viability in kinetochore mutants, premature separation of sister chromatids, and reduction in Cse4p and histone H4 at centromeres. Overexpression of CSE4 or histone H4 suppressed chromosome loss and restored levels of Cse4p at centromeres in GALSCM3 strains. Using mutant alleles of scm3, we identified a domain in the N-terminus of Scm3p that mediates its interaction with CEN DNA and determined that the chromosome loss phenotype of GALSCM3 is due to centromeric association of Scm3p devoid of Cse4p/H4. Furthermore, we determined that similar to other systems the centromeric association of Scm3p is cell cycle regulated. Our results show that altered stoichiometry of Scm3p/HJURP, Cse4p, and histone H4 lead to defects in chromosome segregation. We conclude that stringent regulation of HJURP and SCM3 expression are critical for genome stability.

  4. Microstructure of interaction interface between Al-Si, Zn-Al alloys and Al2O3p/6061Al composite

    许志武; 闫久春; 吕世雄; 杨士勤

    2004-01-01

    Interaction behaviors between Al-Si, Zn-AI alloys and Al2O3p/6061AI composite at different heating temperatures were investigated. It is found that Al2O3p/6061Al composite can be wetted well by AlSi-1, AlSi-4 and Zn-Al alloys and an interaction layer forms between the alloy and composite during interaction. Little Al-Si alloys remain on the surface when they fully wet the composite and Si element in Al-Si alloy diffuses into composite entirely and assembles in the composite near the interface of Al-Si alloy/composite to form a Si-rich zone. The microstructure in interaction layer with Si penetration is still dense. Much more residual Zn-Al alloy exists on the surface of composite when it wets the composite, and porosities appear at the interface of Zn-Al alloy/composite. The penetration of elements Zn, Cu of Zn-Al alloy into composite leads to the generation of shrinkage cavities in the interaction layer and makes the microstructure of Al2 O3p/6061A1 composite loose.

  5. Planarian GSK3s are involved in neural regeneration.

    Adell, Teresa; Marsal, Maria; Saló, Emili

    2008-02-01

    Glycogen synthase kinase-3 (GSK3) is a key element in several signaling cascades that is known to be involved in both patterning and neuronal organization. It is, therefore, a good candidate to play a role in neural regeneration in planarians. We report the characterization of three GSK3 genes in Schmidtea mediterranea. Phylogenetic analysis shows that Smed-GSK3.1 is highly conserved compared to GSK3 sequences from other species, whereas Smed-GSK3.2 and Smed-GSK3.3 are more divergent. Treatment of regenerating planarians with 1-azakenpaullone, a synthetic GSK3 inhibitor, suggests that planarian GSK3s are essential for normal differentiation and morphogenesis of the nervous system. Cephalic ganglia appear smaller and disconnected in 1-azakenpaullone-treated animals, whereas visual axons are ectopically projected, and the pharynx does not regenerate properly. This phenotype is consistent with a role for Smed-GSK3s in neuronal polarization and axonal growth. PMID:18202849

  6. A new form of Ca3P2 with a ring of Dirac nodes

    We report the synthesis and crystal structure of a new high-temperature form of Ca3P2. The crystal structure was determined through Rietveld refinements of synchrotron powder x-ray diffraction data. This form of Ca3P2 has a crystal structure of the hexagonal Mn5Si3 type, with a Ca ion deficiency compared to the ideal 5:3 stoichiometry. This yields a stable, charge-balanced compound of Ca2+ and P3−. We also report the observation of a secondary hydride phase, Ca5P3H, which again is a charge-balanced compound. The calculated band structure of Ca3P2 indicates that it is a three-dimensional Dirac semimetal with a highly unusual ring of Dirac nodes at the Fermi level. The Dirac states are protected against gap opening by a mirror plane in a manner analogous to what is seen for graphene

  7. PbS/Cd3P2 quantum heterojunction colloidal quantum dot solar cells

    Here, we demonstrated the quantum heterojunction colloidal quantum dot (CQD) solar cells employing the PbS CQDs/Cd3P2 CQDs architecture in which both the p-type PbS and n-type Cd3P2 CQD layers are quantum-tunable and solution-processed light absorbers. We synthesized well-crystallized and nearly monodispersed tetragonal Cd3P2 CQDs and then engineered their energy band alignment with the p-type PbS by tuning the dot size and hence the bandgap to achieve efficient light absorbing and charge separation. We further optimized the device through the Ag-doping strategy of PbS CQDs that may leverage an expanded depletion region in the n-layer, which greatly enhances the photocurrent. The resulting devices showed an efficiency of 1.5%. (paper)

  8. Doubly excited 2s2p 1,3p1 resonances in photoionization of helium

    Wan Jian-Jie; Dong Chen-Zhong

    2009-01-01

    The multi-configuration Dirac-Fock (MCDF) method is implemented to study doubly excited 2s2p 1,3P1 resonances of the helium atom and the interference between photoionization and photoexcitation autoionization processes.In order to reproduce the total photoionization sprectra,the excited energies from the ground ls2 1 S0 state to the doubly excited 2s2p 1'3P1 states and the relevant Auger decay rates and widths are calculated in detail. Furthermore,the interference profile determined by the so-called Fano parameters q and p2 is also reproduced. Good agreement is found between the present results and other available theoretical and experimental results. This indeed shows a promising way to investigate the Fano resonances in photoionization of atoms within the MCDF scheme,although there are some discrepancies in the present calculations of the 2s2p 3P1 state.

  9. Relativistic effects on the hyperfine structures of 2p4(3P)3p 2Do, 4Do and 4Po in 19F I

    Carette, Thomas; Li, Jiguang; Godefroid, Michel

    2013-01-01

    The hyperfine interaction constants of the 2p4(3P)3p 2Do_{3/2,5/2}, 4Do_{1/2-7/2} and 4Po_{1/2-5/2} levels in neutral fluorine are investigated theoretically. Large-scale calculations are carried out using the multiconfiguration Hartree-Fock (MCHF) and Dirac-Hartree-Fock (MCDHF) methods. In the framework of the MCHF approach, the relativistic effects are taken into account in the Breit-Pauli approximation using non relativistic orbitals. In the fully relativistic approach, the orbitals are optimized using the Dirac-Coulomb Hamiltonian with correlation models inspired by the non relativistic calculations. Higher-order excitations are captured through multireference configuration interaction calculations including the Breit interaction. In a third (intermediate) approach, the Dirac-Coulomb-Breit Hamiltonian matrix is diagonalized in a relativistic configuration space built with non relativistic MCHF radial functions converted into Dirac spinors using the Pauli approximation. The magnetic dipole hyperfine struct...

  10. Single gene microdeletions and microduplication of 3p26.3 in three unrelated families

    Kashevarova, Anna A; Nazarenko, Lyudmila P; Schultz-Pedersen, Soren; Skryabin, Nikolay A; Salyukova, Olga A; Chechetkina, Nataliya N; Tolmacheva, Ekaterina N; Rudko, Aleksey A; Magini, Pamela; Graziano, Claudio; Romeo, Giovanni; Joss, Shelagh; Tümer, Zeynep; Lebedev, Igor N

    2014-01-01

    BACKGROUND: Detection of submicroscopic chromosomal alterations in patients with a idiopathic intellectual disability (ID) allows significant improvement in delineation of the regions of the genome that are associated with brain development and function. However, these chromosomal regions usually...... contain several protein-coding genes and regulatory elements, complicating the understanding of genotype-phenotype correlations. We report two siblings with ID and an unrelated patient with atypical autism who had 3p26.3 microdeletions and one intellectually disabled patient with a 3p26.3 microduplication...

  11. MiR-373-3p Promotes Invasion and Metastasis of Lung Adenocarcinoma Cells

    Wu, Aibing; Jinmei LI; Kunpeng WU; Mo, Yanli; Luo, Yiping; Haiyin YE; Shen, Xiang; Li, Shujun; Yahai LIANG; Liu, Meilian; Yang, Zhixiong

    2015-01-01

    Background and objective Lung cancer is the leading cause of cancer-related deaths worldwide, and metastasis is the major cause of death in lung cancer patients. MiR-373 is closely associated with invasion and metastasis in other tumor cells. This study explored the expression of miR-373-3p in non-small cell lung cancer (NSCLC) and its effect on the invasive and metastatic capabilities of lung adenocarcinoma cells, as well as their mechanisms of action. Methods The expression of miR-373-3p in...

  12. Domain architectures of the Scm3p protein provide insights into centromere function and evolution

    Aravind, L.; Lakshminarayan, M. Iyer; Wu, Carl

    2007-01-01

    Recently, Scm3p has been shown to be a nonhistone component of centromeric chromatin that binds stoichiometrically to CenH3–H4 histones, and to be required for the assembly of kinetochores in S. cerevisiae. Scm3p is conserved across fungi, and displays a remarkable variation in protein size, ranging from ~200 amino acids in Saccharomyces cerevisiae to ~1300 amino acids in Neurospora crassa. This is primarily due a variable C-terminal segment that is linked to a conserved N-terminal, CenH3-int...

  13. Chromosome 3p microsatellite allelotyping in neuroblastoma: a report on the technical hurdles.

    Hoebeeck, Jasmien; De Wilde, Bram; Michels, Evi; Combaret, Valérie; Yigit, Nurten; De Smet, Els; Van Roy, Nadine; Stanbridge, Eric; Ru, Ning; Laureys, Geneviève; De Paepe, Anne; Speleman, Frank; Vandesompele, Jo

    2009-10-01

    Pinpointing critical regions of recurrent loss may help localize tumor suppressor genes. To determine the regions of loss on chromosome 3p in neuroblastoma, we performed loss of heterozygosity analysis using 16 microsatellite markers in a series of 65 primary tumors and 29 neuroblastoma cell lines. In this study, we report the results and discuss the technical hurdles that we encountered during data generation and interpretation that are of relevance for current studies or tests employing microsatellites. To provide functional support for the implication of 3p tumor suppressor genes in this childhood malignancy, we performed a microcell-mediated chromosome 3 transfer in neuroblastoma cells. PMID:19544108

  14. User access to the MAP3S source emissions inventory

    Benkovitz, C M; Evans, V A

    1981-03-01

    An emissions inventory based on data obtained from the National Emissions Data System (NEDS), the Federal Power Commission (FPC), Environment Canada, and other agencies was compiled by the MAP3S Central Data Coordination at Brookhaven National Laboratory. Pertinent data was brought together, collated, and loaded into computerized data bases using SYSTEM 2000 as the data base management system. These data bases are available to interested users for interactive scanning or batch retrieval. The emissions inventory consists of two distinct sections: a point source inventory and an area source inventory. The point source inventory covers the continental US and Canada; information is kept at the individual source level. The area source inventory covers the continental US; information is kept on a county basis. Work is in progress to obtain a Canadian area source inventory based on census divisions.

  15. Oxidation Behavior of a Pd43Cu27Ni10P20 Bulk Metallic Glass and Foam in Dry Air

    Kai, W.; Ren, I. F.; Barnard, B.; Liaw, P. K.; Demetriou, M. D.; Johnson, W. L.

    2010-07-01

    The oxidation behavior of both Pd43Cu27Ni10P20 bulk metallic glass (Pd4-BMG) and its amorphous foam containing 45 pct porosity (Pd4-AF) was investigated over the temperature range of 343 K (70 °C) to 623 K (350 °C) in dry air. The results showed that virtually no oxidation occurred in the Pd4-BMG at T Cu3P, and Pd3P.

  16. Linkage of atopic dermatitis to chromosomes 4q22, 3p24 and 3q21

    Christensen, Ulla; Møller-Larsen, Steffen; Nyegaard, Mette;

    2009-01-01

    Atopic dermatitis (AD) is a common, itchy skin disease of complex inheritance characterized by dermal and epidermal inflammation. The heritability is considerable and well documented. To date, four genome scans have examined the AD phenotype, showing replicated linkage at 3p26-22, 3q13-21 and 18q11...

  17. Canine-Origin G3P[3] Rotavirus Strain in Child with Acute Gastroenteritis

    De Grazia, Simona; Martella, Vito; Giammanco, Giovanni M; Gòmara, Miren Iturriza; Ramirez, Stefania; Cascio, Antonio; Colomba, Claudia; Arista, Serenella

    2007-01-01

    Infection by an animal-like strain of rotavirus (PA260/97) was diagnosed in a child with gastroenteritis in Palermo, Italy, in 1997. Sequence analysis of VP7, VP4, VP6, and NSP4 genes showed resemblance to a G3P[3] canine strain identified in Italy in 1996. Dogs are a potential source of human viral pathogens.

  18. miR-141-3p inhibits human stromal (mesenchymal) stem cell proliferation and differentiation

    Qiu, Weimin; Kassem, Moustapha

    2014-01-01

    Wnt signaling determines human stromal (mesenchymal) stem cell (hMSC) differentiation fate into the osteoblast or adipocyte lineage. microRNAs (miRNAs) are small RNA molecules of 21-25 nucleotides that regulate many aspects of osteoblast biology. Thus, we examined miRNAs regulated by Wnt signaling...... in hMSC. We identified miRNA (miR)-141-3p as a Wnt target which in turn inhibited Wnt signaling. Moreover, miR-141-3p inhibited hMSC proliferation by arresting cells at the G1 phase of the cell cycle. miR-141-3p inhibited osteoblast differentiation of hMSC as evidenced by reduced alkaline phosphatase...... activity, gene expression and in vitro mineralized matrix formation. Bioinformatic studies, Western blot analysis and 3'UTR reporter assay demonstrated that cell division cycle 25A (CDC25A) is a direct target of miR-141-3p. siRNA-mediated knock-down of CDC25A inhibited hMSC proliferation and osteoblast...

  19. $\\beta$3p- spectroscopy and P-$\\gamma$ width determination in the decay of $^{31}$Ar

    We propose to perform a detailed study of the $\\beta$-decay of the dripline nucleus $^{31}$Ar. This will allow a detailed study of the $\\beta$-delayed 3p-decay as well as provide important information on the resonances of $^{30}$S and $^{29}$P, in particular the ratio between the P- and $\\gamma$- partial widths relevant for astrophysics.

  20. Electron impact investigation of the 3p-Rydberg transitions of acetone

    High resolution (15 meV), gas phase, electron impact energy loss spectra of acetone, and acetone-d6 measured as a function of incident energy and scattering angle have been used to study the anomalously weak 7.4 eV 3p-Rydberg transition in acetone. Assignments made on the basis of isotope shifts and differential electron scattering cross sections show that the weak transition observed optically and in the high energy electron impact spectrum is a forbidden transition to the out-of-plane 3p-Rydberg orbital. The band system is built on a vibronically allowed false origin enabled by the ν23 (CO bend) vibration. The analogous transition in the less symmetric molecule methyl ethyl ketone was observed to be optically allowed. All observed bands could be assigned to the one electronic transition to the out-of-plane 3p-Rydberg orbital. The other two 3p-Rydberg transitions do not appear to be active in acetone or methyl ethyl ketone. An unusual feature of this investigation was the experimental investigation of the relative differential scattering cross sections of both true and false vibronic origins within a single electronic transition. The high energy resolution allowed isotopic substitution, a traditional technique of optical spectroscopy, to be used to establish assignments in an electron impact experiment

  1. miR-200a-3p regulates TLR1 expression in bacterial challenged miiuy croaker.

    Wang, Yanjin; Xu, Guoliang; Han, Jingjing; Xu, Tianjun

    2016-10-01

    MicroRNAs (miRNAs) are highly conserved, small non-coding RNAs which post-transcriptionally regulate various biological processes by repressing mRNA translation or degradating mRNA. It has been demonstrated that miRNAs play crucial roles in regulating the immune system. In this study, we explored the potential roles of miR-200a-3p in regulating TLR signaling pathway in miiuy croaker. Bioinformatics analysis showed that miiuy croaker TLR1 (mmiTLR1) was a putative target of miR-200a-3p. Negative expression profiles in spleen of Vibrio anguillarum challenged miiuy croaker and in lipopolysaccharide (LPS) stimulated miiuy croaker leukocytes further validated the prediction. Luciferase reporter assays showed that the dual-luciferase reporter fused to the 3'UTR of wild type mmiTLR1 cotransfected with miR-200a-3p mimics exhibited a reduction in luciferase activity compared with the controls. All of the present data provide direct evidence that miR-200a-3p is involved in TLR1 expression modulation in miiuy croaker, which will offer a basis for better understanding of miRNA regulation in fish TLR signaling pathways. PMID:27288848

  2. miR-511-3p Modulates Genetic Programs of Tumor-Associated Macrophages

    Mario Leonardo Squadrito

    2012-02-01

    Full Text Available Expression of the mannose receptor (MRC1/CD206 identifies macrophage subtypes, such as alternatively activated macrophages (AAMs and M2-polarized tumor-associated macrophages (TAMs, which are endowed with tissue-remodeling, proangiogenic, and protumoral activity. However, the significance of MRC1 expression for TAM's protumoral activity is unclear. Here, we describe and characterize miR-511-3p, an intronic microRNA (miRNA encoded by both mouse and human MRC1 genes. By using sensitive miRNA reporter vectors, we demonstrate robust expression and bioactivity of miR-511-3p in MRC1+ AAMs and TAMs. Unexpectedly, enforced expression of miR-511-3p tuned down the protumoral gene signature of MRC1+ TAMs and inhibited tumor growth. Our findings suggest that transcriptional activation of Mrc1 in TAMs evokes a genetic program orchestrated by miR-511-3p, which limits rather than enhances their protumoral functions. Besides uncovering a role for MRC1 as gatekeeper of TAM's protumoral genetic programs, these observations suggest that endogenous miRNAs may operate to establish thresholds for inflammatory cell activation in tumors.

  3. 3P2-3F2 pairing in dense neutron matter: the spectrum of solutions

    The 3P2-3F2 pairing model is generally considered to provide an adequate description of the superfluid states of neutron matter at densities some 2-3 times that of saturated symmetrical nuclear matter. The problem of solving the system of BCS gap equations expressing the 3P2-3F2 model is attacked with the aid of the separation approach. This method, developed originally for quantitative study of S-wave pairing in the presence of strong short-range repulsions, serves effectively to reduce the coupled, singular, nonlinear BCS integral equations to a set of coupled algebraic equations. For the first time, sufficient precision becomes accessible to resolve small energy splittings between the different pairing states. Adopting a perturbative strategy, we are able to identify and characterize the full repertoire of real solutions of the 3P2-3F2 pairing model, in the limiting regime of small tensor-coupling strength. The P-F channel coupling is seen to lift the striking parametric degeneracies revealed by a earlier separation treatment of the pure, uncoupled 3P2 pairing problem. Remarkably, incisive and robust results are obtained solely on the basis of analytic arguments. Unlike the traditional Ginzburg-Landau approach, the analysis is not restricted to the immediate vicinity of the critical temperature, but is equally reliable at zero temperature. Interesting connections and contrasts are drawn between triplet pairing in dense neutron matter and triplet pairing in liquid 3He

  4. Atomic parameters for the 2{p}^{5}3p\\;{}^{2}{[3/2]}_{2}-2{p}^{5}3s\\;{}^{2}{[3/2]}_{2}^{o} transition of Ne I relevant in nuclear physics

    Li, Jiguang; Godefroid, Michel; Wang, Jianguo

    2016-06-01

    We calculated the magnetic dipole hyperfine interaction constants and the electric field gradients of 2{p}53p{}2{[3/2]}2 and 2{p}53s{}2[3/2{]}2o levels of Ne I by using the multiconfiguration Dirac–Hartree–Fock method. The electronic factors contributing to the isotope shifts were also estimated for the λ =614.5 {{nm}} transition connecting these two states. Electron correlation and relativistic effects including the Breit interaction were investigated in detail. Combining with recent measurements, we extracted the nuclear quadrupole moment values for 20Ne and 23Ne with a smaller uncertainty than the current available data. Isotope shifts in the 2{p}53p{}2{[3/2]}2-2{p}53s{}2[3/2{]}2o transition based on the present calculated field- and mass-shift parameters are in good agreement with the experimental values. However, the field shifts in this transition are two or three orders of magnitude smaller than the mass shifts, making rather difficult to deduce changes in nuclear-charge mean-square radii. According to our theoretical predictions, we suggest using instead transitions connecting levels arising from the 2p53s configuration to the ground state, for which the normal mass shift and specific mass shift contributions counteract each other, producing relatively small mass shifts that are only one order of magnitude larger than relatively large field shifts, especially for the 2{p}53s{}2[1/2{]}1o-2{p}6{}1{S}0 transition.

  5. Wetland resources investigation based on 3S technology

    Lin, Hui; Jing, Haitao; Zhang, Lianpeng

    2008-10-01

    Wetland is a special ecosystem between land and water . It can provide massive foods, raw material, water resources and habitat for human being, animals and plants, Wetlands are so important that wetlands' development, management and protection have become the focus of public attention ."3S" integration technology was applied to investigate wetland resources in Shandong Province ,the investigation is based on remote sensing(RS) information, combining wetlandrelated geographic information system(GIS) data concerning existing geology, hydrology, land, lakes, rivers, oceans and environmental protection, using the Global Positioning System (GPS) to determine location accurately and conveniently , as well as multi-source information to demonstrate each other based on "3S" integration technology. In addition, the remote sensing(RS) interpretation shall be perfected by combining house interpretation with field survey and combining interpretation results with known data.By contrasting various types of wetland resources with the TM, ETM, SPOT image and combining with the various types of information, remote sensing interpretation symbols of various types of wetland resources are established respectively. According to the interpretation symbols, we systematically interpret the wetland resources of Shandong Province. In accordance with the purpose of different work, we interpret the image of 1987, 1996 and 2000. Finally, various interpretation results are processed by computer scanning, Vectored, projection transformation and image mosaic, wetland resources distribution map is worked out and wetland resources database of Shandong Province is established in succession. Through the investigation, wetland resource in Shandong province can be divided into 4 major categories and 17 sub-categories. we have ascertained the range and area of each category as well as their present utilization status.. By investigating and calculating, the total area of wetland in Shandong Province is

  6. 3S-R10 automated RBS system

    Norton, G. A.; Schroeder, J. B.; Klody, G. M.; Strathman, M. D.

    1989-04-01

    The NEC 3S-R10 automated RBS spectrometer system includes the features required for routine application of Rutherford backscattering (RBS) and related techniques for materials analysis in both research and industrial settings. The NEC Model 3SDH Pelletron accelerator system provides stable, monoenergetic beams of helium ions up to 3.3 MeV and protons to 2.2 MeV and has heavy ion capability. The analytical end station is the fully computerized Charles Evans & Associates Model RBS-400. Automated features include sample positioning (precision 4-axis goniometer), channeling alignment, polar plot generation, and data acquisition and reduction. Computer automation of accelerator and chamber functions includes storage and recall of operating parameters. Unattended data acquisition, e.g., overnight or over a weekend, is possible for up to 100 samples per batch for random orientation, rotating random or channeling analyses at any sample location. Single samples may be up to 50 cm in diameter. A laser for sample alignment and a TV for video monitoring are included. Simultaneous detection (up to 4 detectors) at normal and grazing angles, external control of grazing angle detector position, and transmission scattering capability enhance system flexibility. The system is also compatible with PIXE, NRA, and hydrogen forward-scattering analyses. Data reduction is part of the computer system, which features displays (several formats) and manipulation of up to five spectra at one time using constant multipliers or point by point operations between spectra.

  7. The Euratom Treaty and the 3S approach

    The 3S concept concerns the adoption of an approach by national authorities to legislation and regulation in the areas of nuclear safety, security, and safeguards which treats these closely related areas in an integrated fashion, rather than as three separate Islands. The benefits from adopting such an integrated approach lire the avoidance of legislative or regulatory gaps, and what is equally important: the avoidance of legislative or regulatory overlaps - particularly where conflicts may be concerned. The European Union possesses extensive legislative competences in relation to protecting the health and safety of workers and the public against Ionizing radiation. It also possesses competences in relation to ensuring that nuclear materials are not diverted from their declared uses. In both of these areas there is a nexus with the security of nuclear materials end radioactive materials more generally. The European Commission is currently elaborating a legislative proposal to consolidate the European Basic Standards legislation, which includes the Directive on the control of High Activity Sealed Sources, into a single, integrated legal Instrument. This paper also takes note of current activities in the area of safeguards, which although intended to improve safeguards controls, are also expected to improve security of nuclear materials in the EU. The paper also briefly analyses overlaps between safeguards and safety. (author)

  8. On the magnetocrystalline anisotropy of greigite (Fe3S4)

    Winklhofer, Michael; Chang, Liao; Eder, Stephan H. K.

    2014-04-01

    ferrimagnetic mineral greigite (cubic Fe3S4) is well known as an intracellular biomineralization product in magnetic bacteria and as a widely occurring authigenic mineral in anoxic sediments. Due to the lack of suitable single-crystal specimens, the magnetic anisotropy parameters of greigite have remained poorly constrained, to the point where not even the easy axis of magnetization is known. Here we report on an effort to determine the anisotropy parameters on the basis of ferromagnetic resonance (FMR) powder spectroscopy on hydrothermally synthesized, chemically pure greigite microcrystals dispersed in a nonmagnetic matrix. In terms of easy axis orientations, the FMR data are consistent with or , or less likely, a more general type. With a g factor of 2.09, the anisotropy field is about 90 mT and in some samples may reach 125 mT, compared to 30 mT for cubic magnetite. This confirms the dominating role of cubic anisotropy on the magnetic properties of greigite, which we show to be responsible for large SIRM/k values. K1 is in the range -15 … -23 J/m3 () or +10 … +15 kJ/m3 (), yielding upper limits of 44 or 34 nm for the superparamagnetic grain size, respectively.

  9. Current challenges with understanding greigite (Fe3S4) magnetism

    Chang, L.; Roberts, A. P.; Winklhofer, M.; Vasiliev, I.; Dekkers, M. J.; Krijgsman, W.

    2014-12-01

    Greigite (Fe3S4) is a widespread authigenic magnetic mineral in anoxic sediments, and is also commonly biosynthesized by magnetotactic bacteria in aqueous environments. Despite the importance of greigite in paleomagnetic and environmental magnetic studies, knowledge of its magnetic properties is at a much lower level than for more common rock-forming magnetic minerals. Much recent progress has been made to develop a more complete understanding of the magnetic properties of greigite and the range of grain sizes in which greigite occurs in nature. We present results of new determinations of a range of fundamental magnetic properties of greigite, including the saturation magnetization, the magnetocrystalline anisotropy, and calculated rock magnetic properties. In addition, we provide evidence for the preservation of greigite magnetofossils in ancient sediments, which has important implications for assessing the reliability of paleomagnetic records carried by greigite. Finally, we present an integrated study from a Messinian former Black Sea sedimentary sequence to unravel environmental controls on diagenetic greigite formation, and demonstrates the usefulness of greigite for studying long-term climate variability in anoxic environments.

  10. The valence band electronic structure of the Cu(111) (√3X√3)R30deg-Si interface

    Full text: The structure and bonding of the copper-silicon interface is of considerable interest from a number of aspects. Firstly as a catalyst in the commercial synthesis of silane polymers, secondly as an anti-corrosion treatment, and thirdly, the formation of a well ordered and reactive silicon layer, which can be oxidised is relevant in the creation of ultra-thin silicon oxide-metal interfaces for electronic devices. Silicon is capable of forming a number of compounds with copper, the most widely studied of which is Cu3Si. Calculations have shown that when silicon impurity atoms are incorporated into a copper solid, there is an interaction between copper 3d levels and the 3s and sp levels of silicon. The silicon 2p orbitals rehybridise with the copper 3d band to form bonding and antibonding states separated by -4 eV. The resulting compounds have metallic, rather than semiconducting nature, there is charge transfer from copper to silicon and there is an increase in electron density into the silicon valence bands, making silicon more reactive. The splitting of the density of states near the Fermi edge has been measured as 4-5 eV in amorphous copper-silicon alloys, using Si Kβ fluorescence spectroscopy and has also been inferred from the 4 eV splitting of the LV V auger lines in Cu-Si compounds and in copper deposited on Si(100) and Si(111) surfaces. In this study we have used high resolution valence band photoemission spectroscopy to investigate the nature of the silicon valence bands in a well ordered silicon-copper interface. By comparing the valence band spectra of the clean surface and those from the silicon interface, we are able to identify three silicon-derived features which are in agreement with other published data. We suggest that these levels are due to emission from the 3s and 3p levels of Si

  11. Photoelectric characteristics of CH3NH3PbI3/p-Si heterojunction

    Yamei, Wu; Ruixia, Yang; Hanmin, Tian; Shuai, Chen

    2016-05-01

    Organic–inorganic hybrid perovskite CH3NH3PbI3 film is prepared on p-type silicon substrate using the one-step solution method to form a CH3NH3PbI3/p-Si heterojunction. The film morphology and structure are characterized by atomic force microscopy (AFM) and scanning electron microscopy (SEM). The photoelectric properties of the CH3NH3PbI3/p-Si heterojunction are studied by testing the current–voltage (I–V) with and without illumination and capacitance–voltage (C–V) characteristics. It turns out from the I–V curve without illumination that the CH3NH3PbI3/p-Si heterojunction has a rectifier feature with the rectification ratio over 70 at the bias of ±5 V. Also, there appears a photoelectric conversion phenomenon on this heterojunction with a short circuit current (Isc) of 0.16 μA and an open circuit voltage (Voc) of about 10 mV The high frequency C–V characteristic of the Ag/CH3NH3PbI3/p-Si heterojunction turns out to be similar to that of the metal–insulator–semiconductor (MIS) structure, and a parallel translation of the C–V curve along the forward voltage axis is found. This parallel translation means the existence of defects at the CH3NH3PbI3/p-Si interface and positive fixed charges in the CH3NH3PbI3 layer. The defects at the interface of the CH3NH3PbI3/p-Si heterojunction result in the dramatic decline of the Voc. Besides, the C–V test of CH3NH3PbI3 film shows a non-linear dielectric property and the dielectric value is about 4.64 as calculated. Project supported by the Hebei Province Natural Science Foundation of China (No. F2014202184) and the Tianjin Natural Science Foundation of China (No. 15JCZDJC37800).

  12. Parallel 3D Finite Element Particle-in-Cell Simulations with Pic3P

    Candel, A.; Kabel, A.; Lee, L.; Li, Z.; Ng, C.; Schussman, G.; Ko, K.; /SLAC; Ben-Zvi, I.; Kewisch, J.; /Brookhaven

    2009-06-19

    SLAC's Advanced Computations Department (ACD) has developed the parallel 3D Finite Element electromagnetic Particle-In-Cell code Pic3P. Designed for simulations of beam-cavity interactions dominated by space charge effects, Pic3P solves the complete set of Maxwell-Lorentz equations self-consistently and includes space-charge, retardation and boundary effects from first principles. Higher-order Finite Element methods with adaptive refinement on conformal unstructured meshes lead to highly efficient use of computational resources. Massively parallel processing with dynamic load balancing enables large-scale modeling of photoinjectors with unprecedented accuracy, aiding the design and operation of next-generation accelerator facilities. Applications include the LCLS RF gun and the BNL polarized SRF gun.

  13. Gamma-ray irradiation induced bulk photochromism in WO3-P2O5 glass

    Shen, Wei; Baccaro, Stefania; Cemmi, Alessia; Xu, Xiaoqing; Chen, Guorong

    2015-11-01

    In the present work, photochromism of WO3-P2O5 glass under gamma-ray irradiation was reported. As-prepared glass samples with different WO3 content are all optically transparent in the visible wavelength range thanks to the addition of a small amount of oxidizing couple Sb2O3-NaNO3. The photochromic properties are identified by transmission spectra of the glasses before and after irradiation. The results show that the irradiation induced darkening results from the reduction of W6+ to W5+ or W4+. The existence of WO6 clusters in glasses of high WO3 content is proved by XPS, which is the main reason for the obvious photochromic effects. The WO3-P2O5 glass is a promising candidate in gamma-ray sensitive detector.

  14. Omega3P: A Parallel Finite-Element Eigenmode Analysis Code for Accelerator Cavities

    Lee, Lie-Quan; Li, Zenghai; Ng, Cho; Ko, Kwok; /SLAC

    2009-03-04

    Omega3P is a parallel eigenmode calculation code for accelerator cavities in frequency domain analysis using finite-element methods. In this report, we will present detailed finite-element formulations and resulting eigenvalue problems for lossless cavities, cavities with lossy materials, cavities with imperfectly conducting surfaces, and cavities with waveguide coupling. We will discuss the parallel algorithms for solving those eigenvalue problems and demonstrate modeling of accelerator cavities through different examples.

  15. Ca3P2 and other topological semimetals with line nodes and drumhead surface states

    Chan, Y.-H.; Chiu, Ching-Kai; Chou, M. Y.; Schnyder, Andreas P.

    2016-05-01

    As opposed to ordinary metals, whose Fermi surfaces are two dimensional, topological (semi)metals can exhibit protected one-dimensional Fermi lines or zero-dimensional Fermi points, which arise due to an intricate interplay between symmetry and topology of the electronic wave functions. Here, we study how reflection symmetry, time-reversal symmetry, SU(2) spin-rotation symmetry, and inversion symmetry lead to the topological protection of line nodes in three-dimensional semimetals. We obtain the crystalline invariants that guarantee the stability of the line nodes in the bulk and show that a quantized Berry phase leads to the appearance of protected surfaces states, which take the shape of a drumhead. By deriving a relation between the crystalline invariants and the Berry phase, we establish a direct connection between the stability of the line nodes and the drumhead surface states. Furthermore, we show that the dispersion minimum of the drumhead state leads to a Van Hove singularity in the surface density of states, which can serve as an experimental fingerprint of the topological surface state. As a representative example of a topological semimetal, we consider Ca3P2 , which has a line of Dirac nodes near the Fermi energy. The topological properties of Ca3P2 are discussed in terms of a low-energy effective theory and a tight-binding model, derived from ab initio DFT calculations. Our microscopic model for Ca3P2 shows that the drumhead surface states have a rather weak dispersion, which implies that correlation effects are enhanced at the surface of Ca3P2 .

  16. Temperature dependence and mechanism of the reaction between O(3P) and chlorine dioxide

    Colussi, A. J.; Sander, S. P.; Fiedl, R. R.

    1992-01-01

    Second-order rate constants for the decay of O(3P) in excess chlorine dioxide, k(II), were measured as a function of total pressure (20-600 Torr argon) and temperature (248-312 K), using flash photolysis-atomic resonance fluorescence. Results indicate that k(II) is pressure dependent with a value, K(b), that is nonzero at zero pressure, and both the third-order rate constant and k(b) have negative temperature dependences.

  17. The Participative Design of an Endoscopy Facility using Lean 3P.

    Smith, Iain

    2016-01-01

    In the UK, bowel cancer is the second largest cancer killer. Diagnosing people earlier can save lives but demand for endoscopies is increasing and this can put pressure on waiting times. To address this challenge, an endoscopy unit in North East England decided to improve their facilities to increase capacity and create environments that improve the experience of users. This presented a significant opportunity for step change improvement but also a problem in terms of creating designs that meet user requirements whilst addressing structural or space constraints. The Lean design process known as '3P' (standing for the production preparation process) was utilised as a participative design strategy to engage stakeholders in the design of the new department. This involved a time-out workshop (or 3P event) in which Lean and participative design tools were utilised to create an innovative design based on 'point of delivery' (POD) principles. The team created a design that demonstrated an increase in treatment room capacity by 25% and bed capacity by 70% whilst reducing travel distance for patients by 25.8% and staff by 27.1%. This was achieved with an increase in available space of only 13%. The Lean 3P method provided a structured approach for corporate and clinical staff to work together with patient representatives as cross-functional teams. This participative approach facilitated communication and learning between stakeholders about care processes and personal preferences. Lean 3P therefore appears to be a promising approach to improving the healthcare facilities design process to meet user requirements. PMID:27493744

  18. $^3P_2$-$^3F_2$ Pairing in Dense Neutron Matter The Spectrum of Solutions

    Zverev, M V; Khodel, V A

    2003-01-01

    The $^3P_2$-$^3F_2$ pairing model is generally considered to provide an adequate description of the superfluid states of neutron matter at densities some 2-3 times that of saturated symmetrical nuclear matter. The problem of solving the system of BCS gap equations expressing the $^3P_2$-$^3F_2$ model is attacked with the aid of the separation approach. This method, developed originally for quantitative study of S-wave pairing in the presence of strong short-range repulsions, serves effectively to reduce the coupled, singular, nonlinear BCS integral equations to a set of coupled algebraic equations. For the first time, sufficient precision becomes accessible to resolve small energy splittings between the different pairing states. Adopting a perturbative strategy, we are able to identify and characterize the full repertoire of real solutions of the $^3P_2$-$^3F_2$ pairing model, in the limiting regime of small tensor-coupling strength. The P-F channel coupling is seen to lift the striking parametric degeneracie...

  19. Study of the Ne(^3P_2) + CH_3F Electron Transfer Reaction below 1 Kelvin

    Jankunas, Justin; Osterwalder, Andreas

    2014-01-01

    Relatively little is known about the dynamics of electron transfer reactions at low collision energy. We present a study of Penning ionization of ground state methyl fluoride molecules by electronically excited neon atoms in the 13 $\\mu$eV--4.8 meV (150 mK--56 K) collision energy range, using a neutral-neutral merged beam setup. Relative cross sections have been measured for three Ne($^3P_2$)+ CH$_3$F reaction channels by counting the number of CH$_3$F$^+$, CH$_2$F$^+$, and CH$_3^+$ product ions, as a function of relative velocity between the neon and methyl fluoride molecular beams. Experimental cross sections markedly deviate from the Langevin capture model at collision energies above 20 K. The branching ratios are constant. In other words, the chemical shape of the CH$_3$F molecule, as seen by Ne($^3P_2$) atom, appears not to change as the collision energy is varied, in contrast to related Ne($^3P_J$) + CH$_3$X (X=Cl and Br) reactions at higher collision energies.

  20. Phase transitions in Cd3P2 at high pressures and high temperatures

    Yel'kin, F.S.; Sidorov, V.A.; Waskowska, A.;

    2008-01-01

    The high-pressure, high-temperature structural behaviour of Cd3P2 has been studied using electrical resistance measurements, differential thermal analysis, thermo baric analysis and X-ray diffraction. At room temperature, a phase transformation is observed at 4.0 GPa in compression. The experimen......The high-pressure, high-temperature structural behaviour of Cd3P2 has been studied using electrical resistance measurements, differential thermal analysis, thermo baric analysis and X-ray diffraction. At room temperature, a phase transformation is observed at 4.0 GPa in compression....... The experimental zero-pressure bulk modulus of the low-pressure phase is 64.7(7) GPa, which agrees quite well with the calculated value of 66.3 GPa using the tight-binding linear muffin-tin orbital method within the local density approximation. Tentatively, the high-pressure phase has an orthorhombic crystal...... structure with space group Pmmn (#59). The relative volume change at the phase transition is Delta V/V= -5.5%. Amorphization of the sample occurs above 25 GPa. A P-T phase diagram of Cd3P2 has been constructed. A metastable phase is observed at ambient conditions after heating the sample to above 600 K...

  1. Ypq3p-dependent histidine uptake by the vacuolar membrane vesicles of Saccharomyces cerevisiae.

    Manabe, Kunio; Kawano-Kawada, Miyuki; Ikeda, Koichi; Sekito, Takayuki; Kakinuma, Yoshimi

    2016-06-01

    The vacuolar membrane proteins Ypq1p, Ypq2p, and Ypq3p of Saccharomyces cerevisiae are known as the members of the PQ-loop protein family. We found that the ATP-dependent uptake activities of arginine and histidine by the vacuolar membrane vesicles were decreased by ypq2Δ and ypq3Δ mutations, respectively. YPQ1 and AVT1, which are involved in the vacuolar uptake of lysine/arginine and histidine, respectively, were deleted in addition to ypq2Δ and ypq3Δ. The vacuolar membrane vesicles isolated from the resulting quadruple deletion mutant ypq1Δypq2Δypq3Δavt1Δ completely lost the uptake activity of basic amino acids, and that of histidine, but not lysine and arginine, was evidently enhanced by overexpressing YPQ3 in the mutant. These results suggest that Ypq3p is specifically involved in the vacuolar uptake of histidine in S. cerevisiae. The cellular level of Ypq3p-HA(3) was enhanced by depletion of histidine from culture medium, suggesting that it is regulated by the substrate. PMID:26928127

  2. miR-342-3p affects hepatocellular carcinoma cell proliferation via regulating NF-κB pathway

    Zhao, Liang; Zhang, Yubao, E-mail: zhyb880077@sina.com

    2015-02-13

    Recent research indicates that non-coding microRNAs (miRNAs) help regulate basic cellular processes in many types of cancer cells. We hypothesized that overexpression of miR-342-3p might affect proliferation of hepatocellular carcinoma (HCC) cells. After confirming overexpression of miR-342-3p with qRT-PCR, MTT assay showed that HCC cell proliferation was significantly inhibited by miR-342-3p, and that it significantly decreased BrdU-positive cell proliferation by nearly sixfold. Searching for targets using three algorithms we found that miR-342-3p is related to the NF-κB pathway and luciferase assay found that IKK-γ, TAB2 and TAB3 are miR-342-3p target genes. Results of western blot on extracted nuclear proteins of HepG2 and HCT-116 cells showed that miR-342-3p reduced and miR-342-3p-in increased p65 nuclear levels and qRT-PCR found that NF-κB pathway downstream genes were downregulated by miR-342-3p and upregulated by miR-342-3p-in, confirming that miR-342 targets NF-κB pathway. Overexpression of Ikk-γ, TAB2 and TAB3 partially rescued HCC cells proliferation inhibited by miR-342-3p. Using the GSE54751 database we evaluated expression from 10 HCC samples, which strongly suggested downregulation of miR-342-3p and we also found inverse expression between miR-342-3p and its targets IKK-γ, TAB2 and TAB3 from 71 HCC samples. Our results show that miR-342-3p has a significant role in HCC cell proliferation and is suitable for investigation of therapeutic targets. - Highlights: • MiR-342-3p suppresses hepatocellular carcinoma cell proliferation. • MiR-342-3p targets IKK-γ, TAB2 and TAB3 genes. • MiR-342-3p downregulates NF-kB signaling pathway. • MiR-342-3p is downregulated in clinical hepatocellular carcinoma samples. • The expression of miR-342-3p and its target gene is inversely related.

  3. miR-342-3p affects hepatocellular carcinoma cell proliferation via regulating NF-κB pathway

    Recent research indicates that non-coding microRNAs (miRNAs) help regulate basic cellular processes in many types of cancer cells. We hypothesized that overexpression of miR-342-3p might affect proliferation of hepatocellular carcinoma (HCC) cells. After confirming overexpression of miR-342-3p with qRT-PCR, MTT assay showed that HCC cell proliferation was significantly inhibited by miR-342-3p, and that it significantly decreased BrdU-positive cell proliferation by nearly sixfold. Searching for targets using three algorithms we found that miR-342-3p is related to the NF-κB pathway and luciferase assay found that IKK-γ, TAB2 and TAB3 are miR-342-3p target genes. Results of western blot on extracted nuclear proteins of HepG2 and HCT-116 cells showed that miR-342-3p reduced and miR-342-3p-in increased p65 nuclear levels and qRT-PCR found that NF-κB pathway downstream genes were downregulated by miR-342-3p and upregulated by miR-342-3p-in, confirming that miR-342 targets NF-κB pathway. Overexpression of Ikk-γ, TAB2 and TAB3 partially rescued HCC cells proliferation inhibited by miR-342-3p. Using the GSE54751 database we evaluated expression from 10 HCC samples, which strongly suggested downregulation of miR-342-3p and we also found inverse expression between miR-342-3p and its targets IKK-γ, TAB2 and TAB3 from 71 HCC samples. Our results show that miR-342-3p has a significant role in HCC cell proliferation and is suitable for investigation of therapeutic targets. - Highlights: • MiR-342-3p suppresses hepatocellular carcinoma cell proliferation. • MiR-342-3p targets IKK-γ, TAB2 and TAB3 genes. • MiR-342-3p downregulates NF-kB signaling pathway. • MiR-342-3p is downregulated in clinical hepatocellular carcinoma samples. • The expression of miR-342-3p and its target gene is inversely related

  4. Identification of miR-508-3p and miR-509-3p that are associated with cell invasion and migration and involved in the apoptosis of renal cell carcinoma

    Zhai, Qingna [Department of Clinical Laboratory, Peking University Shenzhen Hospital, Guangdong (China); Shantou University Medical College, Guangdong (China); Zhou, Liang [Guangdong and Shenzhen Key Laboratory of Male Reproductive Medicine and Genetics, Peking University Shenzhen Hospital, Guangdong (China); Zhao, Chunjuan [Department of Clinical Laboratory, Peking University Shenzhen Hospital, Guangdong (China); Shantou University Medical College, Guangdong (China); Wan, Jun [Section of Biochemistry and Cell Biology, Division of Life Science, The Hong Kong University of Science and Technology (Hong Kong); Yu, Zhendong, E-mail: zhendongyu66@hotmail.com [Department of Clinical Laboratory, Peking University Shenzhen Hospital, Guangdong (China); Guo, Xin; Qin, Jie; Chen, Jing [Guangdong and Shenzhen Key Laboratory of Male Reproductive Medicine and Genetics, Peking University Shenzhen Hospital, Guangdong (China); Lu, Ruijing [Department of Clinical Laboratory, Peking University Shenzhen Hospital, Guangdong (China); Shantou University Medical College, Guangdong (China)

    2012-03-23

    Highlights: Black-Right-Pointing-Pointer Previous method was the second-generation sequencing technology. Black-Right-Pointing-Pointer miR-508-3p and miR-509-3p were significantly down-regulated in RCC tissues. Black-Right-Pointing-Pointer They can inhibit cell proliferation and migration and promote cell apoptosis. Black-Right-Pointing-Pointer The expression of miR-508-3p was significantly decreased in RCC patients plasma. Black-Right-Pointing-Pointer miR-508-3p may be a novel diagnostic marker of RCC. -- Abstract: MicroRNAs (miRNAs) have emerged as powerful regulators of multiple processes linked to human cancer, including cell apoptosis, proliferation and migration, suggesting that the regulation of miRNA function could play a critical role in cancer progression. Recent studies have found that human serum/plasma contains stably expressed miRNAs. If they prove indicative of disease states, miRNAs measured from peripheral blood samples may be a source for routine clinical detection of cancer. Our studies showed that both miR-508-3p and miR-509-3p were down-regulated in renal cancer tissues. The level of miR-508-3p but not miR-509-3p in renal cell carcinoma (RCC) patient plasma demonstrated significant differences from that in control plasma. In addition, the overexpression of miR-508-3p and miR-509-3p suppressed the proliferation of RCC cells (786-0), induced cell apoptosis and inhibited cell migration in vitro. Our data demonstrated that miR-508-3p and miR-509-3p played an important role as tumor suppressor genes during tumor formation and that they may serve as novel diagnostic markers for RCC.

  5. Identification of miR-508-3p and miR-509-3p that are associated with cell invasion and migration and involved in the apoptosis of renal cell carcinoma

    Highlights: ► Previous method was the second-generation sequencing technology. ► miR-508-3p and miR-509-3p were significantly down-regulated in RCC tissues. ► They can inhibit cell proliferation and migration and promote cell apoptosis. ► The expression of miR-508-3p was significantly decreased in RCC patients plasma. ► miR-508-3p may be a novel diagnostic marker of RCC. -- Abstract: MicroRNAs (miRNAs) have emerged as powerful regulators of multiple processes linked to human cancer, including cell apoptosis, proliferation and migration, suggesting that the regulation of miRNA function could play a critical role in cancer progression. Recent studies have found that human serum/plasma contains stably expressed miRNAs. If they prove indicative of disease states, miRNAs measured from peripheral blood samples may be a source for routine clinical detection of cancer. Our studies showed that both miR-508-3p and miR-509-3p were down-regulated in renal cancer tissues. The level of miR-508-3p but not miR-509-3p in renal cell carcinoma (RCC) patient plasma demonstrated significant differences from that in control plasma. In addition, the overexpression of miR-508-3p and miR-509-3p suppressed the proliferation of RCC cells (786-0), induced cell apoptosis and inhibited cell migration in vitro. Our data demonstrated that miR-508-3p and miR-509-3p played an important role as tumor suppressor genes during tumor formation and that they may serve as novel diagnostic markers for RCC.

  6. Spectra of identified high-p(T) pi(+/-) and p((p)over-bar ) in Cu + Cu collisions at root s(NN)=200 GeV

    Abelev, B. I.; Aggarwal, M. M.; Ahammed, Z.; Alakhverdyants, A. V.; Anderson, B. D.; Arkhipkin, D.; G.S. Averichev; Balewski, J.; Barnby, L.S.; Baumgart, S.; Beavis, D.R.(Brookhaven National Laboratory, Upton, NY, 11973, USA); Bellwied, R.; Benedosso, F.; Betancourt, M. J.; Betts, R. R.

    2010-01-01

    We report new results on identified (anti) proton and charged pion spectra at large transverse momenta (3 < p(T) < 10 GeV/c) from Cu + Cu collisions at root s(NN) = 200 GeV using the STAR detector at the Relativistic Heavy Ion Collider (RHIC). This study explores the system size dependence of two novel features observed at RHIC with heavy ions: the hadron suppression at high-p(T) and the anomalous baryon to meson ...

  7. Theoretical study of intramultiplet transitions in collisions of atoms in 3P electronic states with structureless targets: Ca(3P)+He

    The quantum close-coupling (CC) treatment of collisions of an atom in a 3P electronic state with a structureless target is developed, based on earlier work of Mies [Phys. Rev. A 7, 942 (1973)], and a j/sub z/-conserving [coupled-states (CS)] simplification presented. There is no direct coupling between the J = 0 and J = 1 levels; transitions between these levels will occur only as a result of Coriolis coupling involving the J = 2 state. Actual CC and CS calculations are reported for collisions of Ca 43P/sup o/ with He, based on the potential curves of Malvern [J. Phys. B 11, 831 (1978)]. In the CC results, of the three independent cross sections, J = 2→1 is predicted to be largest, and J = 2→0 smallest, over the entire range of collision energies sampled. By contrast, the CS approximation predicts the 1→0 transition to be forbidden, and yields only fair accuracy for the CC 2→1 and 2→0 transitions. The coupling between spin-orbit states is also interpreted within an adiabatic model. A comparison with the experimental results of Yuh and Dagdigian (preceding paper) is made by averaging the CC cross sections over the experimental translational energy distribution. The experimental cross sections for the 2→1 and 2→0 transitions are 3--4 times larger than the theoretical values, and the 2→0 cross section is found experimentally to be approx.3 times larger than the 1→0 cross section, in direct contrast with the theoretical prediction for this ratio

  8. Dsj meson decay in the C{sup 3}P{sub 0} model

    Silva, D.T. da; Silva, M.L.L. da; Quadros, J.N. de; Vasconcellos, C.A.Z.; Hadjimichef, D. [Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, RS (Brazil)

    2010-07-01

    Full text. Fock-Tani is a field theory formalism appropriated for the simultaneous treatment of composite particles and their constituents. The formalism was originally developed for the treatment of problems in atomic physics and it was extended later on to the treatment of problems on hadron physics. In the Fock-Tani formalism one starts with the Fock representation of the system using field operators of elementary constituents which satisfy canonical (anti) commutation relations. Composite-particle field operators are linear combinations of the elementary-particle operators and do not generally satisfy canonical (anti) commutation relations. 'Ideal' field operators acting on an enlarged Fock space are then introduced in close correspondence with the composite ones. Next, a given unitary transformation, which transforms the single composite states into single ideal states, is introduced. Application of the unitary operator on the microscopic Hamiltonian, or on other hermitian operators expressed in terms of the elementary constituent field operators, gives equivalent operators which contain the ideal field operators. The effective Hamiltonian in the new representation has a clear physical interpretation in terms of the processes it describes. Since all field operators in the new representation satisfy canonical (anti)commutation relations, the standard methods of quantum field theory can then be readily applied. For a long time the pair creation models for strong hadronic decays have been formulated. The {sup 3}P{sub 0} model is typical decay model which considers only OZI-allowed strong decays. The {sup 3}P{sub 0} model considers a quark-antiquark par creation in the presence of the initial state meson. The quark-antiquark par is created with the vacuum quantum numbers. This model can also be obtained from the non-relativistic limit of the pair creation Hamiltonian. Applying the Fock-Tani transformation to the pair creation Hamiltonian produces the

  9. MiR-142-3p is a RANKL-dependent inducer of cell death in osteoclasts.

    Fordham, Jezrom B; Guilfoyle, Katherine; Naqvi, Afsar Raza; Nares, Salvador

    2016-01-01

    MicroRNA are small, non-coding, single-stranded RNAs that are estimated to regulate ~60% of the human genome. MiRNA profiling of monocyte-to-osteoclast differentiation identified miR-142-3p as a miRNA that is significantly, differentially expressed throughout osteoclastogenesis. Enforced expression of miR-142-3p via transient transfection with miR-142-3p mimic inhibited cell-to-cell contact and fusion, decreased protein kinase C alpha expression, and ultimately reduced cell viability. miR-142-3p was also identified as significantly differentially expressed during monocyte-to-macrophage differentiation and overexpression of miR-142-3p prevented their conversion to osteoclasts. Furthermore, the inhibitory effect of miR-142-3p on osteoclastogenesis extended to the conversion of a third osteoclast precursor cell type- dendritic cells. These results demonstrate miR-142-3p to be a negative regulator of osteoclastogenesis from the 3 main precursor cell types: monocytes, macrophages and dendritic cells. Importantly, decreased survival was dependent upon both miR-142-3p expression and RANK-signaling, with no harmful effects detected in the absence of this combination. As such, miR-142-3p represents a novel target for the selective removal of osteoclasts by targeting of osteoclastogenic pathways. PMID:27113904

  10. MicroRNA-409-3p inhibits osteosarcoma cell migration and invasion by targeting catenin-δ1.

    Wu, Shifeng; Du, Xinjie; Wu, Manwu; Du, Hechun; Shi, Xiaoliang; Zhang, Tao

    2016-06-10

    Osteosarcoma is the most common primary bone cancer which is associated with early metastatic potential and poor prognosis. However, the molecular mechanisms underlying osteosarcoma progression are not well characterized. Here, we investigated the role of miR-409-3p in osteosarcoma metastasis. Osteosarcoma tissue showed decreased expression of miR-409-3p compared to adjacent non-tumorous tissue. The expression level of miR-409-3p was negatively correlated with osteosarcoma metastasis. Overexpression of miR-409-3p in osteosarcoma cells (U2OS) inhibited cell migration and invasion. Bioinformatics analysis showed that catenin-δ1 (CTNND1, p120-catenin) is a direct target of miR-409-3p. Overexpression of miR-409-3p repressed the expression of catenin-δ1 in U2OS cells at both mRNA and protein levels. Meanwhile, miR-409-3p repressed the activity of luciferase reporter containing the 3'-untranslated region (3'UTR) of CTNND1 gene. Furthermore, expression of catenin-δ1 rescued the inhibitory effect of miR-409-3p on cell migration and invasion. Altogether, these results indicated that miR-409-3p targets catenin-δ1 to repress osteosarcoma metastasis. PMID:26992637

  11. Quantum chaos in ultracold collisions between Yb($^1$S$_0$) and Yb($^3$P$_2$)

    Green, Dermot G; Frye, Matthew D; Morita, Masato; Hutson, Jeremy M

    2015-01-01

    We calculate and analyze Feshbach resonance spectra for ultracold Yb($^1$S$_0$) + Yb($^3$P$_2$) collisions as a function of an interatomic potential scaling factor $\\lambda$ and external magnetic field. We show that, at zero field, the resonances are distributed randomly in $\\lambda$, but that signatures of quantum chaos emerge as a field is applied. The random zero-field distribution arises from superposition of structured spectra associated with individual total angular momenta. In addition, we show that the resonances in magnetic field in the experimentally accessible range 400 to 2000~G are chaotically distributed, with strong level repulsion that is characteristic of quantum chaos.

  12. Photoionization from the excited (3p, 3d, 4s, 4p) states of sodium

    Calculations are presented for the total cross section (σ) and the angular distribution of asymmetry parameter (β) for photoionization from initial excited (3p, 3d, 4s and 4p) states of sodium atom. Comparison of our results for σ and β is made with other available theoretical calculations and the experimental data. We also present results for the angular distributions in electron-Na+ elastic scattering at energies of k 0.5 and 1.0 a0. (author). 43 refs., 7 figs., 2 tabs

  13. Gene-centric Association Mapping of Chromosome 3p implicates MST1 in IBD pathogenesis

    Goyette, Philippe; Ng, Aylwin; Lefebvre, Céline; Brant, Steven R.; Cho, Judy H; Duerr, Richard H.; Silverberg, Mark S; Kent D. Taylor; Latiano, Anna; Aumais, Guy; Deslandres, Colette; Jobin, Gilles; Annese, Vito; Daly, Mark J.; Xavier, Ramnik J.

    2008-01-01

    Association mapping and candidate gene studies within IBD linkage regions, as well as genome-wide association studies in CD have led to the discovery of multiple risk genes, but these only explain a fraction of the genetic susceptibility observed in IBD. We have thus been pursuing a region on chromosome 3p21-22 showing linkage to CD and UC using a gene-centric association mapping approach. We identified twelve functional candidate genes by searching for literature co-citations with relevant k...

  14. Electron-phonon superconductivity in $A$Pt$_3$P compounds: from weak to strong coupling

    Subedi, Alaska; Ortenzi, Luciano; Boeri, Lilia

    2012-01-01

    We study the newly discovered Pt phosphides $A$Pt$_3$P ($A$=Sr, Ca, La) [ T. Takayama et al. Phys. Rev. Lett. 108, 237001 (2012)] using first-principles calculations and Migdal-Eliashberg theory. Given the remarkable agreement with the experiment, we exclude the charge-density wave scenario proposed by previous first-principles calculations, and give conclusive answers concerning the superconducting state in these materials. The pairing increases from La to Ca and Sr due to changes in the ele...

  15. A quasi-particle description of the M(3,p) models

    Jacob, P.; Mathieu, P

    2005-01-01

    The M(3,p) minimal models are reconsidered from the point of view of the extended algebra whose generators are the energy-momentum tensor and the primary field \\phi_{2,1} of dimension $(p-2)/4$. Within this framework, we provide a quasi-particle description of these models, in which all states are expressed solely in terms of the \\phi_{2,1}-modes. More precisely, we show that all the states can be written in terms of \\phi_{2,1}-type highest-weight states and their phi_{2,1}-descendants. We fu...

  16. Absolute frequency measurement of the 1S0 - 3P0 transition of 171Yb

    Pizzocaro, Marco; Rauf, Benjamin; Bregolin, Filippo; Milani, Gianmaria; Clivati, Cecilia; Costanzo, Giovanni A; Levi, Filippo; Calonico, Davide

    2016-01-01

    We report the absolute frequency measurement of the unperturbed transition 1S0 - 3P0 at 578 nm in 171Yb realized in an optical lattice frequency standard. The absolute frequency is measured 518 295 836 590 863.55(28) Hz relative to a cryogenic caesium fountain with a fractional uncertainty of 5.4x10-16 . This value is in agreement with the ytterbium frequency recommended as a secondary representation of the second in the International System of Units.

  17. Diagnostic value of solitary pulmonary nodules using 99Tm-3P4-RGD2 scintigraphy

    Objective: To investigate the value of 99Tcm-HYNIC-(poly-(ethylene glycol), PEG)4-E (PEG4-c(RGDfK))2 (99Tcm-3P4-RGD2) SPECT imaging in the diagnosis of SPN by visual and semiquantitative analysis.Methods Twenty-one patients (13 men, 8 women; age range 37-77 (58±11) years) with SPN observed on CT were analyzed prospectively. All patients underwent SPECT imaging after administration of 99Tcm-3P4-RGD2 with a dose of (939 ± 118) MBq. The gold standard was based on the histopathological diagnosis of the surgical samples from all recruited patients. The diagnostic performance of CT, SPECT visual and semiquantitative analysis was compared and analyzed with ROC curves. Immunohistochemistry was performed in part of the samples to obtain the information of integrin αvβ3 expression. Informed consent was obtained from all patients. Application of a new radiopharmaceutical was permitted and approved by the local independent Ethics Committee and the Institutional Review Board of the China-Japan Union Hospital. One-way analysis of variance,two-sample t test were used with SPSS 13.0. Results: Among the 21 SPN patients, 15 cases (71%) were diagnosed as malignant, and the other 6 (29%) were benign. T/NT ratio in malignant SPN was higher than that in benign SPN (1.87 ± 0.39 vs 1.41 ± 0.65), but with no statistical significance (t=2.01, P>0.05). The sensitivities for CT, SPECT visual and semiquantitative analysis were 80% (12/15), 100% (15/15) and 100% (15/15) respectively,and the specificity were all 4/6. The AUC was 0.811 (95% CI 58%-95%) for CT, 0.833 (95% CI 61%-96%) for SPECT and 0.844 (95% CI 62%-96%) for T/NT ratios, which showed no statistical significance (F=0.83, P>0.05). Immunohistochemistry confirmed αvβ3 expression in both the malignant and benign nodules which had uptake of 99Tcm-3P4-RGD2 in SPECT imaging. Conclusion: SPECT visual and semiquantitative analysis with 99Tcm-3P4-RGD2 appears to have high sensitivity and consistency in diagnosis of SPN. (authors)

  18. Pulsar Spin-Down by 3P2 Superfluid Neutron with Field Decay

    LUO Xin-Lian; PENG Qiu-He; CHOU Chih-Kang

    2003-01-01

    To describe pulsar spin-down, we present a simple combined torque model that takes into account both the standard magnetic dipole radiation and the electromagnetic radiation from the 3P2 superSuid vortex neutrons inside neutron star. Using an ordinary exponential model for the magnetic field decay, we derive an analytical formulae for pulsar evolution tracks. The pulsar evolution on the P-P diagram is quite different from that of the standard magnetic dipole radiation model, especially when the supernuid torque or Geld decay becomes dominant.

  19. sup 3 P sub 0 study of meson decays in a chiral quark model

    Bonnaz, R; Silvestre-Brac, B; Fernández, F; Valcarce, A

    2001-01-01

    The strong decays of a meson into two mesons are studied in the framework of the sup 3 P sub 0 model. The meson wave functions are determined by means of a realistic chiral quark model constructed in the baryon sector and comparison is made with a traditional potential of 'Coulomb + linear' type. Two different forms for the creation vertex are analyzed. A momentum dependent vertex is proved to be definitively superior. The chiral quark model provides an overall good description of all known transitions and gives results of roughly the same quality as those obtained from phenomenological quark-antiquark potentials.

  20. Study of Υ(3S,2S)→ηΥ(1S) and Υ(3S,2S)→π+π-Υ(1S) hadronic transitions

    BABAR Collection; Lees, J. P.; Poireau, V.; Tisserand, V.; Snoek, H.; et al

    2011-01-01

    We study the Υ(3S,2S)→ηΥ(1S) and Υ(3S,2S)→π+π-Υ(1S) transitions with 122×106Υ(3S) and 100×106Υ(2S) mesons collected by the BABAR detector at the PEP-II asymmetric-energy e+e- collider. We measure B[Υ(2S)→ηΥ(1S)]=(2.39±0.31(stat.)±0.14(syst.))×10-4 and Γ[Υ(2S)→ηΥ(1S)]/Γ[Υ(2S)→π+π-Υ(1S)]=(1.35±0.17(stat.)±0.08(syst.))×10-3. We find no evidence for Υ(3S)→ηΥ(1S) and obtain B[Υ(3S)→ηΥ(1S)

  1. MiR-519d-3p suppresses invasion and migration of trophoblast cells via targeting MMP-2.

    Jie Ding

    Full Text Available Our study was approved by the Medical Ethics Committee of Tang Du Hospital, Fourth Military Medical University and complied strictly with national ethical guidelines. Preeclampsia (PE is a specific clinical disorder characterized by gestational hypertension and proteinuria and is a leading cause of maternal and perinatal mortality worldwide. The miR-519d-3p is upregulated in the maternal plasma of patients with PE which indicates a possible association between this microRNA and the pathogenesis of PE. No studies to date have addressed the effect of miR-519d-3p on the invasion and migration of trophoblast cells. In our study, we found that miR-519d-3p expression was elevated in placental samples from patients with PE. In vitro, overexpression of miR-519d-3p significantly inhibited trophoblast cell migration and invasion, whereas transfection of a miR-519d-3p inhibitor enhanced trophoblast cell migration and invasion. Luciferase assays confirmed that matrix metalloproteinase-2 (MMP-2 is a direct target of miR-519d-3p. Quantitative real-time PCR and western blot assays showed that overexpression of miR-519d-3p downregulated MMP-2 mRNA and protein expression. Knockdown of MMP-2 using a siRNA attenuated the increased trophoblast migration and invasion promoted by the miR-519d-3p inhibitor. In placentas from patients with PE or normal pregnancies, a negative correlation between the expression of MMP-2 and miR-519d-3p was observed using the Pearson correlation and linear regression analysis. Our present findings suggest that upregulation of miR-519d-3p may contribute to the development of PE by inhibiting trophoblast cell migration and invasion via targeting MMP-2; miR-519d-3p may represent a potential predictive and therapeutic target for PE.

  2. A New Case of an Extremely Rare 3p21.31 Interstitial Deletion.

    Lovrecic, Luca; Bertok, Sara; Žerjav Tanšek, Mojca

    2016-05-01

    Interstitial 3p21.31 deletions have been very rarely reported. We describe a 7-year-old boy with global developmental delay, specific facial characteristics, hydronephrosis, and hypothyreosis with a de novo deletion of 3p21.31, encompassing 29 OMIM genes. Despite the wide use of microarrays, no similar case has been reported in the literature so far. Five overlapping cases are deposited in the DECIPHER database, 2 of which have significant overlapping chromosomal aberrations. They both share some phenotypic characteristics with our case, e.g. developmental delay, intellectual disability and facial dysmorphism (arched eyebrows, hypertelorism, low-set ears, and a large nose tip). In addition, loss-of-function mutations in the SETD2 gene (OMIM 612778) of the deleted region have been described in 3 patients, presenting with some similar clinical features, namely overgrowth, intellectual disability, speech delay, hypotonia, autism, and epilepsy. Therefore, SETD2 may explain part of the phenotype in our case. We focused on 3 other genes in the deleted region, based on their known functions, namely CSPG5 (OMIM 606775), PTH1R (OMIM 168468) and SMARCC1 (OMIM 601732), and assessed their potentially important role in describing the patient's phenotype. Additional cases with haploinsufficiency of this region are needed to elucidate further genotype-phenotype correlations. PMID:27385966

  3. Optical potentials for Ne*(3P2,0)-Ar, N2 interactions

    Baudon, J.; Feron, P.; Miniatura, C.; Perales, F.; Reinhardt, J.; Robert, J.; Haberland, H.; Brunetti, B.; Vecchiocattivi, F.

    1991-08-01

    The differential elastic cross sections for Ne*(3P2,0)-Ar and Ne*(3P2,0)-N2 collisions have been measured in crossed beam experiments at 0.064 and 0.318 and at 0.071 and 0.295 eV, collision energies, respectively. These results have been analyzed simultaneously with integral cross sections and total ionization cross sections already available and optical spherical potentials for these two systems have been obtained. These potentials appear to be rather accurate in the distance range from 2.5 to ˜9 and from 3.0 to ˜9 Å for Ne*-Ar and Ne*-N2, respectively. The well depths and equilibrium distances are 5.12 meV and 4.9 Å for Ne*-Ar and 3.56 meV and 5.40 Å for Ne*-N2. The short-range repulsion in both cases exhibits a change in slope which can be correlated with the influence, for the interaction at shorter distances, of the Ne+ core of the metastable atom, which becomes less effective when the intermolecular distance increases. The optical potentials proposed here are given in analytical form suitable for the calculation of dynamical observables of these systems.

  4. A Mixed-Valent Molybdenum Monophosphate with a Layer Structure: KMo 3P 2O 14

    Guesdon, A.; Borel, M. M.; Leclaire, A.; Grandin, A.; Raveau, B.

    1994-03-01

    A new mixed-valent molybdenum monophosphate with a layer structure KMo 3P 2O 14 has been isolated. It crystallizes in the space group P2 1/ m with a = 8.599(2) Å, b = 6.392(2) Å, c = 10.602(1) Å, and β = 111.65(2)°. The layers [Mo 3P 2O 14] ∞ are parallel to (100) and consist of [MoPO 8] ∞ chains running along limitb→ , in which one MoO 6 octahedron alternates with one PO 4 tetrahedron. In fact, four [MoPO 8] ∞ chains share the corners of their polyhedra and the edges of their octahedra, forming [Mo 4P 4O 24] ∞ columns which are linked through MoO 5 bipyramids along limitc→. The K + ions interleaved between these layers are surrounded by eight oxygens, forming bicapped trigonal prisms KO 8. Besides the unusual trigonal bipyramids MoO 5, this structure is also characterized by a tendency to the localization of the electrons, since one octahedral site is occupied by Mo(V), whereas the other octahedral site and the trigonal bipyramid are occupied by Mo(VI). The similarity of this structure with pure octahedral layer structures suggests the possibility of generating various derivatives, and of ion exchange properties.

  5. Controlling the $2p$ Hole Alignment in Neon via the $2s$-$3p$ Fano Resonance

    Heinrich-Josties, Elisabeth; Santra, Robin

    2014-01-01

    We study the state-resolved production of neon ion after resonant photoionization of Ne via the $2s$-$3p$ Fano resonance. We find that by tuning the photon energy across the Fano resonance a surprisingly high control over the alignment of the final $2p$ hole along the polarization direction can be achieved. In this way hole alignments can be created that are otherwise very hard to achieve. The mechanism responsible for this hole alignment is the destructive interference of the direct and indirect (via the autoionizing $2s^{-1}3p$ state) ionization pathways of $2p$. By changing the photon energy the strength of the interference varies and $2p$-hole alignments with ratios up to 19:1 between $2p_0$ and $2p_{\\pm 1}$ holes can be created: an effect normally only encountered in tunnel ionization using strong-field IR pulses. Including spin-orbit interaction does not change the qualitative feature and leads only to a reduction in the alignment by $2/3$. Our study is based on a time-dependent configuration-interactio...

  6. CHARACTERIZATION AND CHROMOSOMAL ASSIGNMENT OF YEAST ARTIFICIAL CHROMOSOMES CONTAINING HUMAN 3P13-P21-SPECIFIC SEQUENCE-TAGGED SITES

    MICHAELIS, SC; BARDENHEUER, W; LUX, A; SCHRAMM, A; GOCKEL, A; SIEBERT, R; WILLERS, C; SCHMIDTKE, K; TODT, B; VANDERHOUT, AH; BUYS, CHCM; HEPPELLPARTON, AC; RABBITTS, PH; UNGAR, S; SMITH, D; LEPASLIER, D; COHEN, D; OPALKA, B; SCHUTTE, J

    1995-01-01

    Human chromosomal region 3p12-p23 is proposed to harbor at least three tumor suppressor genes involved in the development of lung cancer, renal cell carcinoma, and other neoplasias. In order to identify one of these genes we defined sequence tagged sites (STSs) specific for 3p13-p24.2 by analyzing a

  7. Research of Interaction Between Zn Based Solders and Cu, Al Substrates

    Prach Michal; Kostolný Igor; Koleňák Roman

    2014-01-01

    The paper deals with the study of interaction between Cu, Al substrates (purity 5N) and ZnAl4, ZnAg6Al6 zinc solders for higher application temperatures. Soldering was performed with power ultrasound in the air without flux application at temperature 420 °C. Acting time of ultrasonic vibration was 3 s and ultrasound frequency was 40 kHz. Soldered joints were assessed by optical light microscopy and EDX microanalysis. Intermetallic layers (IM) CuZn4 and Cu5Zn8 were formed at the Cu/ZnAl4 bound...

  8. Interaction between 4p photoionization and 3p resonant excitation channels of krypton

    Complete text of publication follows. The angular distribution of Kr 4p photoelectrons was measured employing a linearly polarized photon beam at energies from 205 eV to 230 eV. In this range the Kr 3p→ns/md (n,m=4,5,6, etc.) resonances can be excited. The experimental anisotropy parameters (β, γ and δ) were determined for the Kr 4p shell and its fine structure components. The measurement was carried out at beamline BW3 of the DORIS III synchrotron light source at HASYLAB (Hamburg, Germany). The ESA-22D electrostatic electron spectrometer was used to analyze the emitted electrons. The spectrometer consists of a spherical and a cylindrical mirror analyzer. The spherical mirror focuses the electrons from the scattering plane to the entrance slit of the cylindrical analyzer performing the energy analysis of the electrons. (For detailed description of an ESA- 22-type electron spectrometer see Ref. [1].) The measured dipole anisotropy parameters ? of Kr 4p photoelectrons are shown in Fig. 1 as a function of photon energy. Resonance-like structure can be seen in the photon energy dependence of the dipole parameters. This structure indicates that the channel interactions are important between the 3p resonant excitation-autoionization and 4p direct photoionization processes in krypton. The natural line width of the 3p photoelectron peaks was determined from the measured spectra and it is about 0.8 eV while the experimental width of the resonance near 220 eV photon energy (3p1/2-1→5s resonant excitation) is approximately 2 eV in Fig. 1. This broadening can be explained with the strong interference between the ionization and excitation channels. As before, we conclude that the angular distribution of photoelectrons is strongly influenced by the excitation processes. Acknowledgements. The authors wish to thank the DORIS III staff for providing excellent working conditions. This work was supported by the NKTH-OTKA (Grant No. K67719), and by the European Community

  9. Unified interpretation of Hund's first and second rules for 2p and 3p atoms.

    Oyamada, Takayuki; Hongo, Kenta; Kawazoe, Yoshiyuki; Yasuhara, Hiroshi

    2010-10-28

    A unified interpretation of Hund's first and second rules for 2p (C, N, O) and 3p (Si, P, S) atoms is given by Hartree-Fock (HF) and multiconfiguration Hartree-Fock (MCHF) methods. Both methods exactly satisfy the virial theorem, in principle, which enables one to analyze individual components of the total energy E(=T+V(en)+V(ee)), where T, V(en), and V(ee) are the kinetic, the electron-nucleus attraction, and the electron-electron repulsion energies, respectively. The correct interpretation for each of the two rules can only be achieved under the condition of the virial theorem 2T+V=0 by investigating how V(en) and V(ee) interplay to attain the lower total potential energy V(=V(en)+V(ee)). The stabilization of the more stable states for all the 2p and 3p atoms is ascribed to a greater V(en) that is caused by contraction of the valence orbitals accompanied with slight expansion of the core orbitals. The contraction of the valence orbitals for the two rules is a consequence of reducing the Hartree screening of the nucleus at short interelectronic distances. The reduced screening in the first rule is due to a greater amount of Fermi hole contributions in the state with the highest total spin-angular momentum S. The reduced screening in the second rule is due to the fact that two valence electrons are more likely to be on opposite sides of the nucleus in the state with the highest total orbital-angular momentum L. For each of the two rules, the inclusion of correlation does not qualitatively change the HF interpretation, but HF overestimates the energy difference ∣ΔE∣ between two levels being compared. The magnitude of the correlation energy is significantly larger for the lower L states than for the higher L states since two valence electrons in the lower L states are less likely to be on opposite sides of the nucleus. The MCHF evaluation of ∣ΔE∣ is in excellent agreement with experiment. The present HF and MCHF calculations demonstrate the above statements

  10. Functional Expression and Characterization of Schizosaccharomyces pombe Avt3p as a Vacuolar Amino Acid Exporter in Saccharomyces cerevisiae.

    Soracom Chardwiriyapreecha

    Full Text Available In Saccharomyces cerevisiae, Avt3p and Avt4p mediate the extrusion of several amino acids from the vacuolar lumen into the cytosol. SpAvt3p of Schizosaccharomyces pombe, a homologue of these vacuolar amino acid transporters, has been indicated to be involved in spore formation. In this study, we confirmed that GFP-SpAvt3p localized to the vacuolar membrane in S. pombe. The amounts of various amino acids increased significantly in the vacuolar pool of avt3Δ cells, but decreased in that of avt3+-overexpressing avt3Δ cells. These results suggest that SpAvt3p participates in the vacuolar compartmentalization of amino acids in S. pombe. To examine the export activity of SpAvt3p, we expressed the avt3+ gene in S. cerevisiae cells. We found that the heterologously overproduced GFP-SpAvt3p localized to the vacuolar membrane in S. cerevisiae. Using the vacuolar membrane vesicles isolated from avt3+-overexpressing S. cerevisiae cells, we detected the export activities of alanine and tyrosine in an ATP-dependent manner. These activities were inhibited by the addition of a V-ATPase inhibitor, concanamycin A, thereby suggesting that the activity of SpAvt3p is dependent on a proton electrochemical gradient generated by the action of V-ATPase. In addition, the amounts of various amino acids in the vacuolar pools of S. cerevisiae cells were decreased by the overproduction of SpAvt3p, which indicated that SpAvt3p was functional in S. cerevisiae cells. Thus, SpAvt3p is a vacuolar transporter that is involved in the export of amino acids from S. pombe vacuoles.

  11. MicroRNA-490-3p inhibits proliferation of A549 lung cancer cells by targeting CCND1

    Highlights: • We examined the level of miR-490-3p in A549 lung cancer cells compared with normal bronchial epithelial cell line. • We are the first to show the function of miR-490-3p in A549 lung cancer cells. • We demonstrate CCND1 may be one of the targets of miR-490-3p. - Abstract: MicroRNAs (miRNAs) are small non-coding RNAs that negatively regulate the translation of messenger RNAs by binding their 3′-untranslated region (3′UTR). In this study, we found that miR-490-3p is significantly down-regulated in A549 lung cancer cells compared with the normal bronchial epithelial cell line. To better characterize the role of miR-490-3p in A549 cells, we performed a gain-of-function analysis by transfecting the A549 cells with chemically synthesized miR-490-3P mimics. Overexpression of miR-490-3P evidently inhibits cell proliferation via G1-phase arrest. We also found that forced expression of miR-490-3P decreased both mRNA and protein levels of CCND1, which plays a key role in G1/S phase transition. In addition, the dual-luciferase reporter assays indicated that miR-490-3P directly targets CCND1 through binding its 3′UTR. These findings indicated miR-490-3P could be a potential suppressor of cellular proliferation

  12. Mechanisms and Kinetics of Radical Reaction of O(1D,3P) + HCN System

    HUANG Yu-Cheng; DU Jin-Yan; JU Xue-Hai; YE Shi-Yong; ZHOU Tao

    2008-01-01

    The reaction of HCN with O(1D, 3P) radical has been investigated by density functional theory (DFT) and ab initio methods. The stationary points on the reaction paths(reactants, intermediates and products) were optimized at the (U)B3LYP/aug-cc-pVTZ level.Single-point calculations were performed at the (U)QCISD(T)/aug-cc-pVTZ level for the optimized structures and all the total energies were corrected by zero-point energy. It is shown that there exist three competing mechanisms of oxygen attacking nitrogen O→N, oxygen attacking carbon O→C and oxygen attacking hydrogen O→H. The rate constants were obtained via Eyring transition-state theory in the temperature range of 600~2000 K. The linear relationship between lnk and 1/T was presented. The results show that path 1 is the main reaction channel and the product of NCO + H is predominant.

  13. High strength Al–Al2O3p composites: Optimization of extrusion parameters

    Luan, B.F.; Hansen, Niels; Godfrey, A.;

    2011-01-01

    Composite aluminium alloys reinforced with Al2O3p particles have been produced by squeeze casting followed by hot extrusion and a precipitation hardening treatment. Good mechanical properties can be achieved, and in this paper we describe an optimization of the key processing parameters. The...... investigation of their mechanical properties and microstructure, as well as on the surface quality of the extruded samples. The evaluation shows that material with good strength, though with limited ductility, can be reliably obtained using a production route of squeeze casting, followed by hot extrusion and a...... precipitation hardening treatment. For the extrusion step optimized processing parameters have been determined as: (i) extrusion temperature=500°C–560°C; (ii) extrusion rate=5mm/s; (iii) extrusion ratio=10:1....

  14. Spin structure of binary processes in the 3P0 model of coloured tube

    The binary processes 0+1/2 →0+1/2 (π-p → π0n, π-p → ηn) are considered in the coloured tube model. It is shown that the relations of residues of the amplitude M0+iσ-vectorn-vectorq/2q0M1 and their q2-dependence at the secondary Regge pole exchange is determined by the wave function of a gg-bar pair which appears in the 3P0 state at disruption of a coloured tube. The account of the Thomas interaction gives a small contribution into matrix elements logarithmically decreasing with energy. The model, accounting for absorption, agrees semiquantitatively with experimental data

  15. Product lambda-doublet ratios for the O(3P) + D2 reaction: A mechanistic imprint

    Jambrina, P G; Aldegunde, J; Brouard, M; Aoiz, F J

    2016-01-01

    In the last decade, the development of theoretical methods have allowed chemists to reproduce and explain almost all of the experimental data associated with elementary atom plus diatom collisions. However, there are still a few examples where theory cannot account yet for experimental results. This is the case for the preferential population of one of the $\\Lambda$-doublet states produced by chemical reactions. In particular, recent measurements of the OD($^2\\Pi$) product of the O($^3$P) + D$_2$ reaction have shown a clear preference for the $\\Pi(A')$ $\\Lambda$-doublet states, in apparent contradiction with {\\em ab initio} calculations, which predict a larger reactivity on the $A"$ potential energy surface. Here we present a method to calculate the $\\Lambda$-doublet ratio when concurrent potential energy surfaces participate in the reaction. It accounts for the experimental $\\Lambda$-doublet populations via explicit consideration of the stereodynamics of the process. Furthermore, our results demonstrate that...

  16. Lanthanide refractory semiconductors based on the Th/sub 3/P/sub 4/ structure

    The phase relationships and the important structural, electrical and thermal properties of the R/sub 3/X/sub 4/-R/sub 2/X/sub 3/ (where R = lanthanides and X = S, Se and Te) phases having the Th/sub 3/P/sub 4/-type structure are reviewed. The room temperature electrical resistivity and Seebeck coefficient of these materials are independent of R and only slightly dependent on X, but critically dependent on the X:R ratio. The long term stability of these phases is also reviewed. Although these materials have good thermoelectric properties there are some problems which need to be solved before these phases can be utilized in thermoelectric devices. These problems include long term stability, higher than desirable thermal conductivities, and low electron mobilities

  17. Precision Hyperfine Structure of 2;^3P State of ^3He with External Magnetic

    Wu, Qixue; Drake, G. W. F.

    2007-06-01

    The theory of the Zeeman effect can be used to extrapolate precise measurements for the fine structure or the hyperfine structure to zero-field strength. In the present work, the hyperfine structure of 2;^3P state of ^3He with external magnetic fields is precisely calculated. The values of the fields for 32 crossings and five anticrossings of the magnetic sublevels are theoretically predicted for magnetic field strengths up to 1 Tesla. The results are compared with experimental work. We include the linear terms, diamagnetic terms, and the 2̂ relativistic correction terms in the Zeeman Hamiltonian. All related matrix elements are calculated with high accuracy by the use of double basis set Hylleraas type variational wave functions[1,2].[1] Z. -C. Yan and G.W.F. Drake, Phys. Rev. A 50, R1980 (1994).[2] Q. Wu and G.W.F. Drake, J. Phys. B 40, 393 (2007).

  18. Electron impact excitation of 2p and 3p states of hydrogen at intermediate energies

    A coupled-channel-optical (CCO) calculation with 9 and 12 atomic states supplemented with the continuum optical potentials for the stronger coupling channels has been performed for the electron impact excitation of hydrogen. The calculated n = 2 and n = 3 differential cross sections and the reduced Stokes parameters are comparable with the state-of-the art calculations. There is closer agreement between the present calculations and the experimental measurements for the reduced Stokes parameters P-bar1 and P-bar3 in the n = 2p excitation at 54.4 eV. The present CCO calculations also display good accord with the limited experimental data for the reduced Stokes parameters in the n = 3p excitation. (authors)

  19. Study of Upsilon(3S,2S) -> eta Upsilon(1S) and Upsilon(3S,2S) -> pi+pi- Upsilon(1S) hadronic trasitions

    The BABAR Collaboration; Lees, J. P.; others

    2011-01-01

    We study the Upsilon(3S,2S)->eta Upsilon(1S) and Upsilon(3S,2S)->pi+pi- Upsilon(1S) transitions with 122 million Upsilon(3S) and 100 million Upsilon(2S) mesons collected by the BaBar detector at the PEP-II asymmetric energy e+e- collider. We measure B[Upsilon(2S)->eta Upsilon(1S)]=(2.39+/-0.31(stat.)+/-0.14(syst.))10^-4 and Gamma[Upsilon(2S)->eta Upsilon(1S)]/Gamma[Upsilon(2S)-> pi+pi- Upsilon(1S)]=(1.35+/-0.17(stat.)+/-0.08(syst.))10^-3. We find no evidence for Upsilon(3S)->eta Upsilon(1S) a...

  20. The spin-spin mixing of 1s3s3S1 and 1s3d3D1 states in the helium isoelectronic sequence

    Both relativistic and nonrelativistic analytical calculations of the off-diagonal matrix elements between excited vertical stroke 1s3s 3S1> and vertical stroke 1s3d 3D1> states of He-like atoms have been performed, taking into account the spin-spin interaction of the first order of perturbation theory. The considered values of nuclear charge Z range from Z = 2 to Z = 100. The nonrelativistic results for neutral helium agree well with earlier numerical estimates. The relativistic approach of evaluation of the off-diagonal matrix elements of He-like multicharged ions is analyzed in some details, using the hydrogen-like approximation for the basis wave functions. A precise evaluation of the one-photon exchange correction to the vertical stroke 1s3s 3S1> and vertical stroke 1s3d 3D1> energies is made. (orig.)

  1. Search For the Lepton-Flavor Violating Decays Y(3S)->e tau and Y(3S)->mu tau

    Aubert, B.

    2008-12-11

    Charged lepton-flavor violating processes are extremely rare in the Standard Model, but they are predicted to occur in several beyond-the-Standard Model theories, including Supersymmetry or models with leptoquarks or compositeness. We present a search for such processes in a sample of 117 x 10{sup 6} {Upsilon}(3S) decays recorded with the BABAR detector. We place upper limits on the branching fractions BF({Upsilon}(3S) {yields} e{sup {+-}}{tau}{sup {-+}}) < 5.0 x 10{sup -6} and BF({Upsilon}(3S) {yields} {mu}{sup {+-}}{tau}{sup {-+}}) < 4.1 x 10{sup -6} at 90% confidence level. These results are used to place lower limits on the mass scale of beyond-the-Standard Model physics contributing to lepton-flavor violating decays of the {Upsilon}(3S).

  2. Microstructure, thermal, and mechanical properties of nanostructured Cu-9.5Ni-4.0Sn-7.5P

    Li, J.; Wang, T. M.

    1995-04-01

    Nanostructured Cu-9.5Ni-4.0Sn-7.5P samples represent a polycrystal microstructure of nanometer-sized α-Cu and Cu3P crystallites for crystallite sizes less than 20 nm and of nanometer-sized α-Cu, Cu3P, and Ni2P crystallites for crystallite sizes greater than 20 nm. The specific heat values between 300 K and 400 K for the nanostructured sample with crystallite size of 10 nm are about 20% higher than for the amorphous sample and about 40% higher than for the coarse-grained sample. The hardness of the nanostructured sample with crystallite size of 10 nm is 30% higher than that of the amorphous sample and 110% higher than that of the coarse-grained sample. The variation in hardness with the crystallite size for the nanostructured samples follows the Hall-Petch relationship.

  3. Thermochemical process for recovering Cu from CuO or CuO.sub.2

    Richardson, deceased, Donald M.; Bamberger, Carlos E.

    1981-01-01

    A process for producing hydrogen comprises the step of reacting metallic Cu with Ba(OH).sub.2 in the presence of steam to produce hydrogen and BaCu.sub.2 O.sub.2. The BaCu.sub.2 O.sub.2 is reacted with H.sub.2 O to form Cu.sub.2 O and a Ba(OH).sub.2 product for recycle to the initial reaction step. Cu can be obtained from the Cu.sub.2 O product by several methods. In one embodiment the Cu.sub.2 O is reacted with HF solution to provide CuF.sub.2 and Cu. The CuF.sub.2 is reacted with H.sub.2 O to provide CuO and HF. CuO is decomposed to Cu.sub.2 O and O.sub.2. The HF, Cu and Cu.sub.2 O are recycled. In another embodiment the Cu.sub.2 O is reacted with aqueous H.sub.2 SO.sub.4 solution to provide CuSO.sub.4 solution and Cu. The CuSO.sub.4 is decomposed to CuO and SO.sub.3. The CuO is decomposed to form Cu.sub.2 O and O.sub.2. The SO.sub.3 is dissolved to form H.sub.2 SO.sub.4. H.sub.2 SO.sub.4, Cu and Cu.sub.2 O are recycled. In another embodiment Cu.sub.2 O is decomposed electrolytically to Cu and O.sub.2. In another aspect of the invention, Cu is recovered from CuO by the steps of decomposing CuO to Cu.sub.2 O and O.sub.2, reacting the Cu.sub.2 O with aqueous HF solution to produce Cu and CuF.sub.2, reacting the CuF.sub.2 with H.sub.2 O to form CuO and HF, and recycling the CuO and HF to previous reaction steps.

  4. Cu(I)/Cu(II) templated functional pseudorotaxanes and rotaxanes

    Subrata Saha; Pradyut Ghosh

    2012-11-01

    Threaded complexes like pseudorotaxanes, rotaxanes based on Cu(I)/Cu(II) ions have shown to be promising for the construction of mechanically interlocked molecular-level architectures. In this short review, we focus on the synthetic strategies developed to construct pseudorotaxanes and rotaxanes using Cu(I)/Cu(II) ions as template. Further, brief discussions on chemical and mechanical properties associated with some of the selected to Cu(I)/Cu(II) based pseudorotaxanes and rotaxanes are presented.

  5. A controllable synthetic route to Cu, Cu2O, and CuO nanotubes and nanorods.

    Cao, Minhua; Hu, Changwen; Wang, Yonghui; Guo, Yihang; Guo, Caixin; Wang, Enbo

    2003-08-01

    Reducing Cu(OH)4(2-) with hydrazine hydrate and glucose in the presence of a structure-directing surfactant at room temperature gave Cu and Cu2O nanotubes/nanorods, respectively, whereas facile hydrothermal treatment of Cu(OH)4(2-) precursor resulted in CuO nanotubes/nanorods. PMID:12932015

  6. Expression of miR-199a-3p in human adipocytes is regulated by free fatty acids and adipokines.

    Gu, Nan; You, Lianghui; Shi, Chunmei; Yang, Lei; Pang, Lingxia; Cui, Xianwei; Ji, Chenbo; Zheng, Wen; Guo, Xirong

    2016-08-01

    Obesity is associated with a notable risk for disease, including risk of cardiovascular disorders, type 2 diabetes mellitus (T2DM) and hypertension. Adipose tissue modulates the metabolism by releasing free fatty acids (FFAs) and adipokines, including leptin, resistin, tumor necrosis factor-α (TNF-α) and interleukin 6 (IL‑6). Altered secretion patterns of FFAs and adipokines have been demonstrated to result in obesity‑associated insulin resistance (IR) and inflammatory responses. MicroRNA-199a-3p (miR)-199a-3p expression is significantly induced in differentiated human adipose-derived mesenchymal stem cells and indicates the association with T2DM. However, the association between miR-199a-3p levels in adipocytes and obesity‑associated IR, as well as inflammatory responses remains to be elucidated. The present study observed an elevation of miR‑199a‑3p expression level in mature human adipocytes (visceral) compared with pre-adipocytes. In addition, miR‑199a‑3p expression was higher in visceral adipose deposits from obese subjects. FFA, TNF-α, IL‑6 and leptin significantly induced miR‑199a‑3p expression in mature human adipocytes, while resistin had the opposite effect. miR‑199a‑3p may represent a factor in the modulation of obesity‑associated IR and inflammatory responses. PMID:27279151

  7. miR-224-3p inhibits autophagy in cervical cancer cells by targeting FIP200.

    Fang, Wang; Shu, Shan; Yongmei, Li; Endong, Zhu; Lirong, Yin; Bei, Sun

    2016-01-01

    Cervical cancer (CC) is a malignant solid tumor, which is one of the main causes of morbidity and mortality in women. Persistent High-risk human papillomavirus (hrHPV) infection is closely related to cervical cancer and autophagy has been suggested to inhibit viral infections. miRNAs have been reported to regulate autophagy in many solid tumors with many studies implicating miR-224-3p in the regulation of autophagy. In this study, we performed a miRNA microarray analysis on CC tissues and found that a large number of miRNAs with differential expressions in hrHPV-infected tissues. We identified miR-224-3p as a candidate miRNA selectively up regulated in HPV-infected tissues and cell lines. Further analysis revealed that miR-224-3p regulates autophagy in cervical cancer tissues and cell lines. While the overexpression of miR-224-3p inhibits autophagy in HPV-infected cells, knocking down endogenous miR-224-3p increases autophagy activity in the same cells. In addition, we found that miR-224-3p directly inhibits the expression of autophagy related gene, FAK family-interacting protein of 200 kDa (FIP200). In summary, we found that miR-224-3p regulates autophagy in hrHPV-induced cervical cancer cells through targeting FIP200 expression. PMID:27615604

  8. miR-208-3p promotes hepatocellular carcinoma cell proliferation and invasion through regulating ARID2 expression

    MicroRNAs (miRNAs) are small non-coding RNAs that negatively regulate gene expression at post-transcriptional level. miRNA dysregulation plays a causal role in cancer progression. In this study, miR-208-3p was highly expressed and directly repressed ARID2 expression. As a result, ARID2 expression in hepatocellular carcinoma (HCC) was decreased. In vitro, miR-208-3p down-regulation and ARID2 over-expression elicited similar inhibitory effects on HCC cell proliferation and invasion. In vivo test results revealed that miR-208-3p down-regulation inhibited HCC tumorigenesis in Hep3B cells. Moreover, ARID2 was possibly a downstream element of transforming growth factor beta1 (TGFβ1)/miR-208-3p/ARID2 regulatory pathway. These findings suggested that miR-208-3p up-regulation is associated with HCC cell progression and may provide a new target for liver cancer treatment. - Highlights: • miR-208-3p was highly expressed and directly repressed the expression of ARID2 in HCC. • miR-208-3p contributed to HCC cell progression both in vitro and in vivo. • Over-expression of ARID2 inhibited the HCC cell proliferation and invasion. • Restoration of ARID2 partly reversed the the effect of miR-208-3p down-regulation on HCC cells. • Newly regulatory pathway: miR-208-3p mediated the repression of ARID2 by TGFβ1 in HCC cells

  9. MicroRNA-23a-3p promotes the development of osteoarthritis by directly targeting SMAD3 in chondrocytes.

    Kang, Liang; Yang, Cao; Song, Yu; Liu, Wei; Wang, Kun; Li, Shuai; Zhang, Yukun

    2016-09-01

    Osteoarthritis (OA) is a common chronic degenerative joint disease. Progressive destruction of the integrity of articular cartilage is an important pathological feature, but treatment options that reverse this damage have not been developed. According to recent studies, microRNAs have important regulatory roles in the initiation and progression of OA. In the current study, the biological effects of miR-23a-3p and its expression in OA tissues were examined. We found that miR-23a-3p expression was obviously higher and SMAD3 expression was significantly lower in OA cartilage than in normal tissues. The hypomethylation status of CpG islands in the promoter region of miR-23a-3p was confirmed by methylation-specific polymerase chain reaction in OA cartilage tissues. Furthermore, a bioinformatics analysis and luciferase reporter assay identified SMAD3 as a target gene of miR-23a-3p and SMAD3 expression at both the protein and mRNA levels was inhibited by miR-23a-3p. A functional analysis demonstrated that miR-23a-3p overexpression suppresses type II collagen and aggrecan expression, while miR-23a-3p inhibition had the opposite effects. Small interfering RNA-mediated knockdown of SMAD3 reversed the effects of the miR-23a-3p inhibitor on the expression of type II collagen and aggrecan. Our results suggested that miR-23a-3p contributes to OA progression by directly targeting SMAD3, providing a potential therapeutic target for OA treatment. PMID:27318087

  10. miR-208-3p promotes hepatocellular carcinoma cell proliferation and invasion through regulating ARID2 expression

    Yu, Peng; Wu, Dingguo; You, Yu; Sun, Jing; Lu, Lele; Tan, Jiaxing; Bie, Ping, E-mail: bieping2010@163.com

    2015-08-15

    MicroRNAs (miRNAs) are small non-coding RNAs that negatively regulate gene expression at post-transcriptional level. miRNA dysregulation plays a causal role in cancer progression. In this study, miR-208-3p was highly expressed and directly repressed ARID2 expression. As a result, ARID2 expression in hepatocellular carcinoma (HCC) was decreased. In vitro, miR-208-3p down-regulation and ARID2 over-expression elicited similar inhibitory effects on HCC cell proliferation and invasion. In vivo test results revealed that miR-208-3p down-regulation inhibited HCC tumorigenesis in Hep3B cells. Moreover, ARID2 was possibly a downstream element of transforming growth factor beta1 (TGFβ1)/miR-208-3p/ARID2 regulatory pathway. These findings suggested that miR-208-3p up-regulation is associated with HCC cell progression and may provide a new target for liver cancer treatment. - Highlights: • miR-208-3p was highly expressed and directly repressed the expression of ARID2 in HCC. • miR-208-3p contributed to HCC cell progression both in vitro and in vivo. • Over-expression of ARID2 inhibited the HCC cell proliferation and invasion. • Restoration of ARID2 partly reversed the the effect of miR-208-3p down-regulation on HCC cells. • Newly regulatory pathway: miR-208-3p mediated the repression of ARID2 by TGFβ1 in HCC cells.