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Sample records for y3940 z3930 x4160

  1. Production of X(4160), Y(3940) and Z(3930) in the B¯0 --> K¯*0X(YZ) and B¯s0 --> phiX(YZ) decays

    Energy Technology Data Exchange (ETDEWEB)

    Liang, Wei-Hong [Guangxi Normal Universitym Guilin, China; Molina, Rachel [George Washington Univ., Washington, DC (United States); Xie, Ju-Jun [Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, China; Doring, Michael [George Washington Univ., Washington, DC (United States); Oset, Eugenio [Centro Mixto Universidad de Valencia-CSIC, Institutos de Investigacio´ n de Paterna, Apartado 22085, 46071 Valencia, Spain

    2016-06-01

    We have investigated the decays of and with R being the X(4160), Y(3940), Z(3930) and a predicted J = 1 resonances. By using a model in which these states are dynamically generated from the vector-vector interaction, most notably the and states, we predicted five ratios for the production of these states. Some ratios show that the resonance is built from c with or without extra hadronization. In order to offer some extra test for the molecular composition of these states, we have evaluated the invariant mass distributions for the and close to threshold and made predictions for these magnitudes relative to the width for the production of the resonances.

  2. Predictions for the anti B0 → anti K*0 X(YZ) and anti Bs0 → φ X(YZ) with X(4160), Y(3940), Z(3930)

    International Nuclear Information System (INIS)

    Liang, Wei-Hong; Molina, R.; Doering, M.; Xie, Ju-Jun; Oset, E.

    2015-01-01

    We investigate the decay of anti B 0 → anti K *0 R and anti B s 0 → φR with R being the X(4160), Y(3940), Z(3930) resonances. Under the assumption that these states are dynamically generated from the vector-vector interaction, as has been concluded from several theoretical studies, we use a reaction mechanism of quark production at the elementary level, followed by hadronization of one final q anti q pair into two vectors and posterior final state interaction of this pair of vector mesons to produce the resonances. With this procedure we are able to predict five ratios for these decays, which are closely linked to the dynamical nature of these states, and also predict the order of magnitude of the branching ratios which we find of the order of 10 -4 , well within the present measurable range. In order to further test the dynamical nature of these resonances we study the anti B s 0 → φ D* anti D* and anti B s 0 → φ D s * anti D s * decays close to the D* anti D* and D s * anti D s * thresholds and make predictions for the ratio of the mass distributions in these decays and the anti B s 0 → φR decay widths. The measurement of these decays rates can help unravel the nature of these resonances. (orig.)

  3. Predictions for the anti B{sup 0} → anti K{sup *0} X(YZ) and anti B{sub s}{sup 0} → φ X(YZ) with X(4160), Y(3940), Z(3930)

    Energy Technology Data Exchange (ETDEWEB)

    Liang, Wei-Hong [Guangxi Normal University, Department of Physics, Guilin (China); Chinese Academy of Sciences, Institute of Modern Physics, Lanzhou (China); Molina, R.; Doering, M. [The George Washington University, Washington, DC (United States); Xie, Ju-Jun [Chinese Academy of Sciences, Institute of Modern Physics, Lanzhou (China); Institute of Modern Physics of CAS and Lanzhou University, Research Center for Hadron and CSR Physics, Lanzhou (China); Institute of Theoretical Physics, Chinese Academy of Sciences, State Key Laboratory of Theoretical Physics, Beijing (China); Oset, E. [Chinese Academy of Sciences, Institute of Modern Physics, Lanzhou (China); Centro Mixto Universidad de Valencia-CSIC Institutos de Investigacion de Paterna, Departamento de Fisica Teorica y IFIC, Valencia (Spain)

    2015-05-15

    We investigate the decay of anti B{sup 0} → anti K{sup *0}R and anti B{sub s}{sup 0} → φR with R being the X(4160), Y(3940), Z(3930) resonances. Under the assumption that these states are dynamically generated from the vector-vector interaction, as has been concluded from several theoretical studies, we use a reaction mechanism of quark production at the elementary level, followed by hadronization of one final q anti q pair into two vectors and posterior final state interaction of this pair of vector mesons to produce the resonances. With this procedure we are able to predict five ratios for these decays, which are closely linked to the dynamical nature of these states, and also predict the order of magnitude of the branching ratios which we find of the order of 10{sup -4}, well within the present measurable range. In order to further test the dynamical nature of these resonances we study the anti B{sub s}{sup 0} → φ D* anti D* and anti B{sub s}{sup 0} → φ D{sub s}{sup *} anti D{sub s}{sup *} decays close to the D* anti D* and D{sub s}{sup *} anti D{sub s}{sup *} thresholds and make predictions for the ratio of the mass distributions in these decays and the anti B{sub s}{sup 0} → φR decay widths. The measurement of these decays rates can help unravel the nature of these resonances. (orig.)

  4. Radiative open charm decay of the Y(3940), Z(3930), X(4160) resonances

    International Nuclear Information System (INIS)

    Liang, W.H.; Molina, R.; Oset, E.

    2010-01-01

    We determine the radiative decay amplitudes for the decay into D * and anti Dγ, or D * s and anti D s γ of some of the charmonium-like states classified as X, Y, Z resonances, plus some other hidden charm states which are dynamically generated from the interaction of vector mesons with charm. The mass distributions as a function of the anti Dγ or anti D s γ invariant mass show a peculiar behavior as a consequence of the D * anti D * nature of these states. The experimental search of these magnitudes can shed light on the nature of these states. (orig.)

  5. Reanalysis of the Y(3940), Y(4140), Zc(4020), Zc(4025), and Zb(10650) as molecular states with QCD sum rules

    International Nuclear Information System (INIS)

    Wang, Zhi-Gang

    2014-01-01

    In this article, we calculate the contributions of the vacuum condensates up to dimension 10 in the operator product expansion, and study the J PC = 0 ++ , 1 +- , 2 ++ D * anti D * , D s * anti D s * , B * anti B * , B s * anti B s * molecular states with the QCD sum rules. In the calculations, we use the formula μ = √(M 2 X/Y/Z -(2M Q ) 2 ) to determine the energy scales of the QCD spectral densities. The numerical results favor assigning the Z c (4020) and Z c (4025) to the J PC = 0 ++ , 1 +- or 2 ++ D * anti D * molecular states, the Y(4140) to the J PC = 0 ++ D s * anti D s * molecular state, the Z b (10650) to the J PC = 1 +- B * anti B * molecular state, and they disfavor assigning the Y(3940) to the (J PC = 0 ++ ) molecular state. The present predictions can be confronted with the experimental data in the future. (orig.)

  6. Study of the states Ds1(2536)+ and Z(3930)

    International Nuclear Information System (INIS)

    Schroeder, Torsten

    2008-02-01

    The electron-positron annihilation events studied in the framework of the BABAR experiment at a c. m. energy of 10.58 GeV represent a rich source for the production of charm-containing resonances. In connection with the excellent instrumentation of the detector a precise measurement of this states becomes possible. In the present thesis a precision measurement of the D s1 (2536) + is performed. 8000 decays of the D s1 (2536) + into D *+ K S 0 are reconstructed. Basing on this the mass and the decay width of the D s1 (2536) + can be determined with high precision. Additionally by a decay-angle analysis the spin-parity of the D s1 (2536) + is determined. In the second part of the thesis the 2-photon production of the Z(2930) is studied in the decay into D anti D. Mass, decay width, and spin-parity of the Z(2930) are measured [de

  7. Radially excited states of η{sub c}

    Energy Technology Data Exchange (ETDEWEB)

    Wang, Hui; Yan, Zhaozhao; Ping, Jialun [Nanjing Normal University, Department of Physics, Jiangsu Key Laboratory for Numerical Simulation of Large Scale Complex Systems, Nanjing (China)

    2015-05-15

    In the framework of chiral quark model, the mass spectrum of η{sub c}(ns) (n = 1,.., 6) is studied with Gaussian expansion method. With the wave functions obtained in the study of the mass spectrum, the open flavor two-body strong decay widths are calculated by using the {sup 3}P{sub 0} model. The results show that the masses of η{sub c}(1S) and η{sub c}(2S) are consistent with the experimental data. The explanation of X(3940) as η{sub c}(3S) is possible because the decay width of η{sub c}(3S) is in the range of the experimental value of X(3940). Although the mass of X(4160) is about 110 MeV less than that of η{sub c}(4S) and the decay width of X(4160) is much larger than that of η{sub c}(4S), the assignment of X(4160) as η{sub c}(4S) cannot be excluded due to the large uncertainty of the experimental decay width and the compatibility of the branching ratios of η{sub c}(4S) with that of X(4160), and the mass of η{sub c}(4S) can be shifted downwards by taking into account the coupling effect of the open charm channels. There are still no good candidates to η{sub c}(5S) and η{sub c}(6S). (orig.)

  8. Radially excited states of η{sub c}

    Energy Technology Data Exchange (ETDEWEB)

    Wang, Hui; Yan, Zhaozhao; Ping, Jialun, E-mail: jlping@njnu.edu.cn [Department of Physics, Jiangsu Key Laboratory for Numerical Simulation of Large Scale Complex Systems, Nanjing Normal University, 210023, Nanjing, People’s Republic of (China)

    2015-05-06

    In the framework of chiral quark model, the mass spectrum of η{sub c}(ns) (n=1,…,6) is studied with Gaussian expansion method. With the wave functions obtained in the study of the mass spectrum, the open flavor two-body strong decay widths are calculated by using the {sup 3}P{sub 0} model. The results show that the masses of η{sub c}(1S) and η{sub c}(2S) are consistent with the experimental data. The explanation of X(3940) as η{sub c}(3S) is possible because the decay width of η{sub c}(3S) is in the range of the experimental value of X(3940). Although the mass of X(4160) is about 110 MeV less than that of η{sub c}(4S) and the decay width of X(4160) is much larger than that of η{sub c}(4S), the assignment of X(4160) as η{sub c}(4S) cannot be excluded due to the large uncertainty of the experimental decay width and the compatibility of the branching ratios of η{sub c}(4S) with that of X(4160), and the mass of η{sub c}(4S) can be shifted downwards by taking into account the coupling effect of the open charm channels. There are still no good candidates to η{sub c}(5S) and η{sub c}(6S)

  9. Prediction of a missing higher charmonium around 4.26 GeV in J/ψ family

    International Nuclear Information System (INIS)

    He, Li-Ping; Chen, Dian-Yong; Liu, Xiang; Matsuki, Takayuki

    2014-01-01

    Inspired by the similarity between the mass gaps of the J/ψ and Υ families, the prediction of a missing higher charmonium with mass 4,263 MeV and very narrow width is made. In addition, the properties of two charmonium-like states, X(3940) and X(4160), and charmonium ψ(4415) are discussed, where our calculation shows that X(3940) as η c (3S) is established, while the explanation of X(4160) to be η c (4S) is fully excluded and that η c (4S) is typically a very narrow state. These predictions might be accessible at BESIII, Belle, and BelleII in near future

  10. Prediction of a missing higher charmonium around 4.26 GeV in J/ψ family

    Energy Technology Data Exchange (ETDEWEB)

    He, Li-Ping; Liu, Xiang [Institute of Modern Physics of CAS, Lanzhou University, Research Center for Hadron and CSR Physics, Lanzhou (China); Lanzhou University, School of Physical Science and Technology, Lanzhou (China); Chen, Dian-Yong [Institute of Modern Physics of CAS, Lanzhou University, Research Center for Hadron and CSR Physics, Lanzhou (China); Institute of Modern Physics of CAS, Nuclear Theory Group, Lanzhou (China); Matsuki, Takayuki [Tokyo Kasei University, Itabashi, Tokyo (Japan); Nishina Center, RIKEN, Theoretical Research Division, Saitama (Japan)

    2014-12-01

    Inspired by the similarity between the mass gaps of the J/ψ and Υ families, the prediction of a missing higher charmonium with mass 4,263 MeV and very narrow width is made. In addition, the properties of two charmonium-like states, X(3940) and X(4160), and charmonium ψ(4415) are discussed, where our calculation shows that X(3940) as η{sub c}(3S) is established, while the explanation of X(4160) to be η{sub c}(4S) is fully excluded and that η{sub c}(4S) is typically a very narrow state. These predictions might be accessible at BESIII, Belle, and BelleII in near future. (orig.)

  11. Prediction of a missing higher charmonium around 4.26 GeV in J/ψ family

    Energy Technology Data Exchange (ETDEWEB)

    He, Li-Ping, E-mail: help08@lzu.edu.cn [Research Center for Hadron and CSR Physics, Institute of Modern Physics of CAS, Lanzhou University, 730000, Lanzhou (China); School of Physical Science and Technology, Lanzhou University, 730000, Lanzhou (China); Chen, Dian-Yong, E-mail: chendy@impcas.ac.cn [Research Center for Hadron and CSR Physics, Institute of Modern Physics of CAS, Lanzhou University, 730000, Lanzhou (China); Nuclear Theory Group, Institute of Modern Physics of CAS, 730000, Lanzhou (China); Liu, Xiang, E-mail: xiangliu@lzu.edu.cn [Research Center for Hadron and CSR Physics, Institute of Modern Physics of CAS, Lanzhou University, 730000, Lanzhou (China); School of Physical Science and Technology, Lanzhou University, 730000, Lanzhou (China); Matsuki, Takayuki, E-mail: matsuki@tokyo-kasei.ac.jp [Tokyo Kasei University, 1-18-1 Kaga, 173-8602, Itabashi, Tokyo (Japan); Theoretical Research Division, Nishina Center, RIKEN, 351-0198, Saitama (Japan)

    2014-12-11

    Inspired by the similarity between the mass gaps of the J/ψ and Υ families, the prediction of a missing higher charmonium with mass 4,263 MeV and very narrow width is made. In addition, the properties of two charmonium-like states, X(3940) and X(4160), and charmonium ψ(4415) are discussed, where our calculation shows that X(3940) as η{sub c}(3S) is established, while the explanation of X(4160) to be η{sub c}(4S) is fully excluded and that η{sub c}(4S) is typically a very narrow state. These predictions might be accessible at BESIII, Belle, and BelleII in near future.

  12. Qq(Q-bar)(q-bar)' states in chiral SU(3) quark model

    International Nuclear Information System (INIS)

    Zhang Haixia; Zhang Min; Zhang Zongye

    2007-01-01

    We study the masses of Qq(Q-bar)(q-bar)' states with J PC =0 ++ , 1 ++ , 1 +- and 2 ++ in the chiral SU(3) quark model, where Q is the heavy quark (c or b) and q(q') is the light quark (u,d or s). According to our numerical results, it is improbable to make the interpretation of [cn(c-bar)(n-bar)] 1 ++ and [cn(c-bar)(n-bar)] 2 ++ (n=u,d) states as X(3872) and Y(3940), respectively. However, it is interesting to find the tetraquarks in the bq(b-bar)(q-bar)' system. (authors)

  13. Quarkonium Spectroscopy And Search for New States at BaBar

    Energy Technology Data Exchange (ETDEWEB)

    Cibinetto, G.

    2011-11-04

    The BaBar experiment at the PEP-II B-factory gives excellent opportunities for the quarkonium spectroscopy. Investigation of the properties of new states like the X(3872), Y(3940) and Y(4260) are performed aiming to understand their nature. Recent BaBar results will be presented in this paper. At the B-factories charmonium and charmonium-like states are copiously produced via several mechanisms: in B decay (color suppressed b {yields} c transition), double charmonium production (e{sup +}e{sup -} {yields} c{bar c} + c{bar c}), two photons production ({gamma}*{gamma}* {yields} c{bar c}, where the c{bar c} state has positive C-parity) and in initial state radiation (ISR) when the e{sup {+-}} in its initial state emits a photon lowering the effective center of mass energy of the e{sup +}e{sup -} interaction (e{sup +}e{sup -} {yields} {gamma}{sub ISR} + c{bar c}, where the charmonium state has the quantum numbers J{sup PC} = 1{sup -2}). Many new states have been recently discovered at the B-factories, BaBar and Belle, above the D{bar D} threshold in the charmonium energy region. While some of them appear to be consistent with conventional c{sub c} states others do not fit with any expectation. Several interpretations for these states have been proposed: for some of them the mass values suggest that they could be conventional charmonia, but also other interpretations like D{sup 0}{bar D}*{sup 0} molecule or diquark-antidiquark states among many other models have been advanced. Reviews can be found in Refs. [1][2]. In all cases the picture is not completely clear. This situation could be remedied by a coherent search of the decay pattern to D{bar D}, search for production in two-photon fusion and ISR, and of course improving the statistical precision upon the current measurements. The BaBar experiment at the PEP-II asymmetric collider, designed to perform precision measurement of CP violation in the B meson system, has an extensive quarkonium spectroscopy program. Recent

  14. Charmonium resonances in the 3.9 GeV/c2 energy region and the X(3915)/X(3930) puzzle

    Science.gov (United States)

    Ortega, Pablo G.; Segovia, Jorge; Entem, David R.; Fernández, Francisco

    2018-03-01

    An interesting controversy has emerged challenging the widely accepted nature of the X (3915) and the X (3930) resonances, which had initially been assigned to the χc0 (2 P) and χc2 (2 P) c c bar states, respectively. To unveil their inner structure, the properties of the JPC =0++ and JPC =2++ charmonium states in the energy region of these resonances are analyzed in the framework of a constituent quark model. Together with the bare q q bar states, threshold effects due to the opening of nearby meson-meson channels are included in a coupled-channels scheme calculation. We find that the structure of both states is dominantly molecular with a probability of bare q q bar states lower than 45%. Our results favor the hypothesis that X (3915) and X (3930) resonances arise as different decay mechanisms of the same JPC =2++ state. Moreover we find an explanation for the recently discovered M = 3860MeV /c2 as a JPC =0++ 2P state and rediscover the lost Y (3940) as an additional state in the JPC =0++ family.

  15. Mass spectra for q c q ¯ c ¯, s c s ¯ c ¯, q b q ¯ ¯, s b s ¯ ¯ tetraquark states with JP C=0++ and 2++

    Science.gov (United States)

    Chen, Wei; Chen, Hua-Xing; Liu, Xiang; Steele, T. G.; Zhu, Shi-Lin

    2017-12-01

    We have studied the mass spectra of the hidden-charm/bottom q c q ¯c ¯, s c s ¯c ¯ and q b q ¯b ¯, s b s ¯b ¯ tetraquark states with JP C=0++ and 2++ in the framework of QCD sum rules. We construct ten scalar and four tensor interpolating currents in a systematic way and calculate the mass spectra for these tetraquark states. The X*(3860 ) may be either an isoscalar tetraquark state or χc 0(2 P ). If the X*(3860 ) is a tetraquark candidate, our results prefer the 0++ option over the 2++ one. The X (4160 ) may be classified as either the scalar or tensor q c q ¯c ¯ tetraquark state, while the X (3915 ) favors a 0++ q c q ¯c ¯ or s c s ¯c ¯ tetraquark assignment over the tensor one. The X (4350 ) cannot be interpreted as a s c s ¯c ¯ tetraquark with either JP C=0++ or 2++.

  16. Quantum field theory approaches to meson structure

    International Nuclear Information System (INIS)

    Branz, Tanja

    2011-01-01

    Meson spectroscopy became one of the most interesting topics in particle physics in the last ten years. In particular, the discovery of new unexpected states in the charmonium spectrum which cannot be simply explained by the constituent quark model attracted the interest of many theoretical efforts. In the present thesis we discuss different meson structures ranging from light and heavy quark-antiquark states to bound states of hadrons-hadronic molecules. Here we consider the light scalar mesons f 0 (980) and a 0 (980) and the charmonium-like Y(3940), Y(4140) and Z ± (4430) states. In the discussion of the meson properties like mass spectrum, total and partial decay widths and production rates we introduce three different theoretical methods for the treatment and description of hadronic structure. For the study of bound states of mesons we apply a coupled channel approach which allows for the dynamical generation of meson-meson resonances. The decay properties of meson molecules are further on studied within a second model based on effective Lagrangians describing the interaction of the bound state and its constituents. Besides hadronic molecules the effective Lagrangian approach is also used to study the radiative and strong decay properties of ordinary quark-antiquark (q anti q) states. The AdS/QCD model forms the completion of the three theoretical methods introduced in the present thesis. This holographic model provides a completely different ansatz and is based on extra dimensions and string theory. Within this framework we calculate the mass spectrum of light and heavy mesons and their decay constants.

  17. Mass spectra of four-quark states in the hidden charm sector

    International Nuclear Information System (INIS)

    Patel, Smruti; Shah, Manan; Vinodkumar, P.C.

    2014-01-01

    Masses of the low-lying four-quark states in the hidden charm sector (cq anti c anti q; q element of u,d) are calculated within the framework of a non-relativistic quark model. The four-body system is considered as two two-body systems such as diquark-antidiquark (Qq- anti Q anti q) and quark-antiquark-quark-antiquark (Q anti q- anti Qq) molecular-like four-quark states. Here, the Cornell-type potential has been used for describing the two-body interactions among Q-q, anti Q- anti q, Q- anti q, Qq- anti Q anti q and Q anti q- anti Qq, with appropriate string tensions. Our present analysis suggests the following exotic states: X(3823), Z c (3900), X(3915), Z c (4025), ψ (4040), Z 1 (4050) and X(4160) as Q anti q- anti Qq molecular-like four-quark states, while Z c (3885), X(3940) and Y(4140) as the diquark-antidiquark four-quark states. We have been able to assign the J PC values for many of the recently observed exotic states according to their structure. Apart from this, we have identified the charged state Z(4430) recently confirmed by LHCb as the first radial excitation of Zc(3885) with G = + 1 and Y(4360) state as the first radial excitation of Y(4008) with G = - 1 and the state ψ(4415) as the first radial excitation of the ψ(4040) state. (orig.)