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Sample records for synchrophasotrons

  1. Polarized deuteron beam at the Dubna synchrophasotron

    International Nuclear Information System (INIS)

    Ershov, V.P.; Fimushkin, V.V.; Gai, G.I.

    1990-01-01

    The experimental equipment and setup used to accelerate a polarized deuteron beam at the Dubna synchrophasotron are briefly described. Basic characteristics of the cryogenic source of polarized deuterons POLARIS are presented. The results of measurements of the intensity of the accelerated beam, vector and tensor polarization at the output of the linac LU-20, inside the synchrophasotron ring and in the extracted beam are given. 16 refs.; 9 figs.; 3 tabs

  2. Signal shape registration in the JINR synchrophasotron slowly extracted beam parameter control system

    International Nuclear Information System (INIS)

    Volkov, V.I.; Kulikov, I.I.; Romanov, S.V.

    1982-01-01

    Signal shape registration in the JINR synchrophasotron slowly estracted beam parameter control system on-line with the ES-1010 computer is described. 32 input signals can be connected to the registrator. The maximum measurement rate of signal shape registration is about 38 kHz. The registrator consists of 32-channel analog multiplexer, 10-bit analog-to-digital converter, 1024-word buffer memory and control circuits. For information representation the colour TV monitor is used

  3. Development of the CAMAC on-line control system for the JINR synchrophasotron

    International Nuclear Information System (INIS)

    Volkov, V.I.; Efimov, L.G.; Issinskij, I.B.

    1978-01-01

    A system for controlling the parameters of slow extraction (SE) of a beam from the JINR synchrophasotron is described. The system is also intended for measuring the parameters of a closed beam orbit, measuring and correcting the SE parameters, and providing for the operator-system dialogue. The main computer is the ES-1010 with memory 32 K of 16 digit words. A program channel connects ES-1010 with a VT 1010B mini-computer with a 16 K memory of 8 digit words. The equipment for measuring the accelerator parameters incorporates: 12-digit analog-to-digital converter, a 50 MHz quartz generator, a binary counter, and a timer. The closed orbit is measured by means of two 8-digit analog-to-digital converters, a control circuit, and a small-capacity buffer memory. Six fast 8-digit analog-to-digital converters, a memory module with capacity for 256 24-digit words and an autonomous control module were developed for measuring the three-dimensional characteristics of the extracted beam in six points of the transportation channel. Control of time characteristics is achieved by means of binary counters, a quartz generator, and a levelling device. The equipment was made in the CAMAC standard, and the programs were written on ASSEMBLER and FORTRAN

  4. Research of the Mass Spectra of the Fission Products and Yields of (n, gamma) and (n, 2n) Reactions in a Model Subcritical Uranium Blanket of the Electronuclear System "Energy Plus Transmutation" on Proton Beam of the Dubna Synchrophasotron at 1.5 Ge

    CERN Document Server

    Chultem, D; Krivopustov, M I; Gerbish, S; Tumendemberel, B; Pavlyuk, A B; Zaveryukha, O S

    2002-01-01

    This paper is devoted to the research of the spatial distributions of the yields of (n, f), (n, gamma) and (n, 2n) reactions in a two-section model of the uranium blanket electronuclear installation constructed at the Laboratory of High Energies, JINR (Dubna) for experiments according to the program "Research of physical aspects of the electronuclear method of energy production and of radioactive waste transmutation in atomic power-engineering on beams of the synchrophasotron and nuclotron" - project "Energy plus Transmutation". The mass spectrum of the fission products and yields of above reactions in uranium activation detectors placed on the radii of the so-called detector plates is determined. The experimental results testify that the fission of nuclei in the uranium blanket is made by fast neutrons. This conclusion coincides with the result obtained with track integrators of uranium fission.

  5. Control of parameters of the beam slow extraction from a synchrophasotron on-line with the ES-1010 and VT-1010B computers

    International Nuclear Information System (INIS)

    Volkov, V.I.; Efimov, L.G.; Issinskij, I.B.; Kolpakov, I.F.; Kulikov, I.I.

    1981-01-01

    Description of the system for beam control during slow extraction from the Dubna synchrotron is presented. The ES-1010 minicomputer is the main computer in the system. Measuring and control of the accele-- rator parameters in the operation mode of slow extraction, of the magnetic field index frequency of the accelerating voltage, intensity of the circulating beam, and spatial characteristics of the extracted beam are conducted by means of the control system. Stabilization of parameters of the extracted beam, monitoring of beams of accelerating nuclei, provision of the operator-computer dialogue are carried out by means of this system. Application of the system at the synchrotron permitted to reduce time of tuning the accelerator modes and improve characteristics of the extracted beams [ru

  6. The movable polarized target as a basic equipment for high energy spin physics experiments at the JINR-Dubna accelerator complex

    Energy Technology Data Exchange (ETDEWEB)

    Lehar, F.; Adiasevich, B.; Androsov, V.P.; Angelov, N.; Anischenko, N.; Antonenko, V.; Ball, J.; Baryshevsky, V.G.; Bazhanov, N.A.; Belyaev, A.A.; Benda, B.; Bodyagin, V.; Borisov, N.; Borzunov, Yu.; Bradamante, F.; Bunyatova, E.; Burinov, V.; Chernykh, E.; Combet, M.; Datskov, A.; Durand, G.; Dzyubak, A.P.; Fontaine, J.M.; Get`man, V.A.; Giorgi, M.; Golovanov, L.; Grebenyuk, V.; Grosnick, D.; Gurevich, G.; Hasegawa, T.; Hill, D.; Horikawa, N.; Igo, G.; Janout, Z.; Kalinnikov, V.A.; Karnaukhov, I.M.; Kasprzyk, T.; Khachaturov, B.A.; Kirillov, A.; Kisselev, Yu.; Kousmine, E.S.; Kovalenko, A.; Kovaljov, A.I.; Ladygin, V.P.; Lazarev, A.; Leconte, P.; Lesquen, A. de; Lukhanin, A.A.; Mango, S.; Martin, A.; Matafonov, V.N.; Matyushevsky, E.; Mironov, S.; Neganov, A.B.; Neganov, B.S.; Nomofilov, A.; Perelygin, V.; Plis, Yu.; Pilipenko, Yu.; Pisarev, I.L.; Piskunov, N.; Polunin, Yu.; Popkov, Yu.P.; Propov, A.A.; Prokofiev, A.N.; Rekalo, M.P.; Rukoyatkin, P.; Sans, J.L.; Sapozhnikov, M.G.; Sharov, V.; Shilov, S.; Shishov, Yu.; Sitnik, I.M.; Sorokin, P.V.; Spinka, H.; Sporov, E.A.; Strunov, L.N.; Svetov, A.; De Swart, J.J.; Telegin, Yu.P.; Tolmashov, I.; Trentalange, S.; Tsvinev, A.; Usov, Yu.A.; Vikhrov, V.V.; Whitten, C.A.; Zaporozhets, S.; Zarubin, A.; Zhdanov, A.A.; Zolin, L. [CEA Centre d`Etudes Nucleaires de Saclay, 91 - Gif-sur-Yvette (France). Dept. d`Astrophysique, de Physique des Particules, de Physique Nucleaire et de l`Instrumentation Associee]|[I.V. Kurchatov Inst. of Atomic Energy, Moscow (Russian Federation)]|[Kharkov Inst. of Physics and Technology (Russian Federation)]|[Lab. of Nuclear Problems, JINR, Dubna (Russian Federation)]|[Lab. of High Energy Physics, JINR, Dubna (Russian Federation)]|[Lab. National SATURNE, CNRS, 91 - Gif-sur-Yvette (France)]|[Inst. of Physics, Belarus Academy of Sciences, Minsk (Belarus)]|[Dept. of Physics, Petersburg Nuclear Physics Inst., Gatchina (Russian Federation)

    1995-03-01

    A movable polarized proton target is planned to be installed in polarized beams of the Synchrophasotron-Nuclotron complex in order to carry out a spin physics experimental program at Dubna. The project is described and the first proposed experiments are discussed. ((orig.))

  7. The movable polarized target as a basic equipment for high energy spin physics experiments at the JINR-Dubna accelerator complex

    International Nuclear Information System (INIS)

    Lehar, F.; Adiasevich, B.; Androsov, V.P.; Angelov, N.; Anischenko, N.; Antonenko, V.; Ball, J.; Baryshevsky, V.G.; Bazhanov, N.A.; Belyaev, A.A.; Benda, B.; Bodyagin, V.; Borisov, N.; Borzunov, Yu.; Bradamante, F.; Bunyatova, E.; Burinov, V.; Chernykh, E.; Combet, M.; Datskov, A.; Durand, G.; Dzyubak, A.P.; Fontaine, J.M.; Get'man, V.A.; Giorgi, M.; Golovanov, L.; Grebenyuk, V.; Grosnick, D.; Gurevich, G.; Hasegawa, T.; Hill, D.; Horikawa, N.; Igo, G.; Janout, Z.; Kalinnikov, V.A.; Karnaukhov, I.M.; Kasprzyk, T.; Khachaturov, B.A.; Kirillov, A.; Kisselev, Yu.; Kousmine, E.S.; Kovalenko, A.; Kovaljov, A.I.; Ladygin, V.P.; Lazarev, A.; Leconte, P.; Lesquen, A. de; Lukhanin, A.A.; Mango, S.; Martin, A.; Matafonov, V.N.; Matyushevsky, E.; Mironov, S.; Neganov, A.B.; Neganov, B.S.; Nomofilov, A.; Perelygin, V.; Plis, Yu.; Pilipenko, Yu.; Pisarev, I.L.; Piskunov, N.; Polunin, Yu.; Popkov, Yu.P.; Propov, A.A.; Prokofiev, A.N.; Rekalo, M.P.; Rukoyatkin, P.; Sans, J.L.; Sapozhnikov, M.G.; Sharov, V.; Shilov, S.; Shishov, Yu.; Sitnik, I.M.; Sorokin, P.V.; Spinka, H.; Sporov, E.A.; Strunov, L.N.; Svetov, A.; De Swart, J.J.; Telegin, Yu.P.; Tolmashov, I.; Trentalange, S.; Tsvinev, A.; Usov, Yu.A.; Vikhrov, V.V.; Whitten, C.A.; Zaporozhets, S.; Zarubin, A.; Zhdanov, A.A.; Zolin, L.

    1995-01-01

    A movable polarized proton target is planned to be installed in polarized beams of the Synchrophasotron-Nuclotron complex in order to carry out a spin physics experimental program at Dubna. The project is described and the first proposed experiments are discussed. ((orig.))

  8. The movable polarized target as a basic equipment for high energy spin physics experiments at the JINR-Dubna accelerator complex

    Science.gov (United States)

    Lehar, F.; Adiasevich, B.; Androsov, V. P.; Angelov, N.; Anischenko, N.; Antonenko, V.; Ball, J.; Baryshevsky, V. G.; Bazhanov, N. A.; Belyaev, A. A.; Benda, B.; Bodyagin, V.; Borisov, N.; Borzunov, Yu.; Bradamante, F.; Bunyatova, E.; Burinov, V.; Chernykh, E.; Combet, M.; Datskov, A.; Durand, G.; Dzyubak, A. P.; Fontaine, J. M.; Get'man, V. A.; Giorgi, M.; Golovanov, L.; Grebenyuk, V.; Grosnick, D.; Gurevich, G.; Hasegawa, T.; Hill, D.; Horikawa, N.; Igo, G.; Janout, Z.; Kalinnikov, V. A.; Karnaukhov, I. M.; Kasprzyk, T.; Khachaturov, B. A.; Kirillov, A.; Kisselev, Yu.; Kousmine, E. S.; Kovalenko, A.; Kovaljov, A. I.; Ladygin, V. P.; Lazarev, A.; Leconte, Ph.; de Lesquen, A.; Lukhanin, A. A.; Mango, S.; Martin, A.; Matafonov, V. N.; Matyushevsky, E.; Mironov, S.; Neganov, A. B.; Neganov, B. S.; Nomofilov, A.; Perelygin, V.; Plis, Yu.; Pilipenko, Yu.; Pisarev, I. L.; Piskunov, N.; Polunin, Yu.; Popkov, Yu. P.; Propov, A. A.; Prokofiev, A. N.; Rekalo, M. P.; Rukoyatkin, P.; Sans, J. L.; Sapozhnikov, M. G.; Sharov, V.; Shilov, S.; Shishov, Yu.; Sitnik, I. M.; Sorokin, P. V.; Spinka, H.; Sporov, E. A.; Strunov, L. N.; Svetov, A.; de Swart, J. J.; Telegin, Yu. P.; Tolmashov, I.; Trentalange, S.; Tsvinev, A.; Usov, Yu. A.; Vikhrov, V. V.; Whitten, C. A.; Zaporozhets, S.; Zarubin, A.; Zhdanov, A. A.; Zolin, L.

    1995-02-01

    A movable polarized proton target is planned to be installed in polarized beams of the Synchrophasotron-Nuclotron complex in order to carry out a spin physics experimental program at Dubna. The project is described and the first proposed experiments are discussed.

  9. Autonomous control unit for CAMAC-branch universal driver

    International Nuclear Information System (INIS)

    Efimov, L.G.; Chernykh, E.V.

    1979-01-01

    An autonomous program control module with an instrumental program used in the multipurpose driver of the CAMAC branch is described. The module is designed to provide rapid acquisition and record, into a buffer storage, of information on spatial characteristics of an extracted beam in the system for control the parameters of slow extraction of the synchrophasotron beam. The module makes it possible to reduce the data acquisition and recording time 9 times and also fast control of operation of proportional chamber electronic circuits

  10. Overload protection device for pulsed electric systems

    International Nuclear Information System (INIS)

    Glushchenko, V.G.; Kurskov, I.A.; Semina, R.S.

    1976-01-01

    Results of pulsed electric system protection development from effective pulse current overload depending on pulse duration are described. An integrating circuit, charge resistance of which is connected in parallel with a stabilitron, is used in a protection diagram. Given were time responses of overload protection of an output lens of slow root particle extraction channel from synchrophasotron; the responses have been obtained by the experimental and calculation methods

  11. JINR-DUBNA an International center of Nuclear Research

    Science.gov (United States)

    Gudima, K.; Baznat, M.

    2015-04-01

    A short History of the Joint Institute of the Nuclear Research in Dubna (Russian Federation) has been given. The Facilities : The Synchrophasotron, the Nuclotron-M, the IBR-2 Reactor,The Heavy Ions Isochronous cyclotrons U-400 and U-400M, Phasotron, The impuls resonance neutronic device IREN has been described. A short history of collaboration between JINR and scientists from Moldova has been given. The main new tendencies in Science management has been outlined.

  12. Particle identification in the MASPIK time-of-flight magnetic spectrometer

    International Nuclear Information System (INIS)

    Azhgirej, L.S.; Zarubin, P.I.; Ivanov, V.V.; Kuznetsov, A.S.; Stoletov, G.D.

    1985-01-01

    Characteristics of the system for time-of-flight measurement in the MASPIK magnetic spectrometer with wire chambers designed for studying the nuclear reaction mechanism in extracted beams of relativistic nuclei at the JINR synchrophasotron are considered. The functional diagram of the utilized equipment and mass distribution of secondary particles detected by the spectrometer in the range of momenta of 5.7-8.5 GeV/s are presented. Pulses from two scintillation detectors placed at the distance of 21.9 m from one another are applied for determining time-of-flight of particles detected by the main arm of the spectrometer. These counters are switched also into the trigger system of the facility. The attained time resolution permits to strictly separate protons and deuterons

  13. Neutron production in spallation reactions of 0.9 and 1.5 GeV protons on a thick lead target. Comparison between experimental data and Monte-Carlo simulations

    International Nuclear Information System (INIS)

    Krasa, A.; Krizek, F.; Wagner, V.; Kugler, A.; Henzl, V.; Henzlova, D.; Majerle, M.; Adam, J.; Caloun, P.; Bradnova, V.; Chultem, D.; Kalinnikov, V.G.; Krivopustov, M.I.; Solnyshkin, A.A.; Stegajlov, V.I.; Tsupko-Sitnikov, V.M.; Tumehndehlgehr, Ts.; Vasil'ev, S.I.

    2005-01-01

    This paper reports on two experiments performed at the Synchrophasotron/Nuclotron accelerator complex at JINR. Relativistic protons with energies 885 MeV and 1.5 GeV hit a massive cylindrical lead target. The spatial and energetic distributions of the neutron field produced by the spallation reactions were measured by the activation of Al, Au, Bi, Co, and Cu foils placed on the surface of the target and close to it. The yields of the radioactive nuclei produced by threshold reactions in these foils were determined by the analyses of their γ spectra. The comparison with Monte-Carlo based simulations was performed both with the LAHET+MCNP code and the MCNPX code

  14. Transmutation studies using SSNTD and radiochemistry and the associated production of secondary neutrons

    CERN Document Server

    Brandt, R; Wan, J S; Schmidt, T; Langrock, E J; Vater, P; Adam, J; Bamblevski, V P; Bradnova, V; Gelovani, L K; Kalinnikov, V K; Krivopustov, M I; Kulakov, B A; Sosnin, A N; Perelygin, V P; Pronskikh, V S; Stegailov, V I; Tsoupko-Sitnikov, V M; Modolo, G; Odoj, R; Philippen, P W; Adloff, J C; Pape, F; Debeauvais, M; Zamani-Valassiadou, M; Hashemi-Nezhad, S R; Dwivedi, K K; Guo Shi Lun; Li, L; Wang, Y L; Wilson, B

    1999-01-01

    Experiments using 1.5 GeV, 3.7 GeV and 7.4 GeV protons from the Synchrophasotron, LHE, JINR, Dubna, Russia, on extended Pb- and U- targets were carried out using SSNTD and radiochemical sensors for the study of secondary neutron $9 fluences. We also carried out first transmutation studies on the long-lived radwaste nuclei /sup 129/I and /sup 237/Np. In addition, we carried out computer code simulation studies on these systems using LAHET and DCM/CEM codes. We $9 have difficulties to understand rather large transmutation rates observed experimentally when they are compared with computer simulations. There seems to be a rather fundamental problem understanding the large transmutation rates as $9 observed experimentally in Dubna and CERN, as compared to those theoretical computer simulations mentioned above. (10 refs).

  15. Experience gained during 10 years transmutation experiments in Dubna

    Science.gov (United States)

    Zamani, M.; Fragopoulou, M.; Manolopoulou, M.; Stoulos, S.; Brandt, R.; Westmeier, W.; Krivopustov, M.; Sosnin, A.; Golovatyuk, S.

    2006-05-01

    Transmutation, the procedure of transforming long-lived radioactive isotopes into stable or short-lived, was proposed for reducing the amount of radioactive waste resulting from technological applications of nuclear fission. The Accelerator Driven Systems (ADS) provide the possibility to generate intense neutron spectrum yielding in an effective transmutation of unwanted isotopes. Such experiments are being carried out for the last 10 years in Synchrophasotron / Nuclotron accelerators at the Veksler-Baldin Laboratory of High Energies of the Joint Institute for Nuclear Research in Dubna, Russia. Thick Pb and Pb-U targets, surrounded by moderators, have been irradiated by protons in the energy range of 0.5-7.4 GeV. Neutron fluence measurements have been performed by different techniques of passive detectors (neutron activation detectors, solid state nuclear track detectors). Transmutation of 129I, 237Np, 239Pu was studied. The results of these experiments are presented and discussed.

  16. Determination of spatial and energy distributions of neutrons in experiments on transmutation of radioactive waste using relativistic protons

    CERN Document Server

    Zhuk, I V; Boulyga, S F; Kievitskaia, A I; Rakhno, I L; Chigrinov, S E; Bradnova, V; Krivopustov, M I; Kulakov, B A; Brandt, R; Ochs, M; Wan, J S

    1999-01-01

    The experiments on transmutation of sup 1 sup 2 sup 9 I and sup 2 sup 3 sup 7 Np using uranium-lead targets surrounded by a paraffin moderator were performed at the Joint Institute for Nuclear Research (JINR, Russia). The targets were irradiated by 1.5 GeV and 7.4 GeV protons at the Synchrophasotron of JINR. In the frame of present work spatial and energy distributions of neutrons on the surface of the paraffin moderator were measured using SSNTD technique. It is shown that measured values of spectral indices do not depend on the energy of incident protons but depend on the target composition. The presence of the uranium insertion softens neutron spectra.

  17. Software and hardware complex on the base of semiconductor detectors operating on-line with the MERA-60/45, ES-1060 and ES-1061 computers

    International Nuclear Information System (INIS)

    Butsev, V.S.; Butseva, G.L.; Nefed'eva, L.S.; Panyutchev, E.I.

    1987-01-01

    The improved software and hardware complex (setup GAMMA) are described in detail. Using these facilities, the fragmentation of projectiles, target-nuclei and production and decay mechanism of radioactive nuclides on beams of relativistic particles and nuclei (p, d, a, 12 C, 16 O) of an energy of 4.5 GeV/nucleon accelerated at the Dubna synchrophasotron have been studied during 1980-1987. The facilities consist of Ge(Li)-detectors CAMAC multichannel analyzers on-line with HP-2116B and MERA-60/45 computers and appropriate software. The facilities are used for the acquisition of spectrometric information, its preliminary processing and transfer to the base BESM-6, ES-1060 and ES-1061 computers. A problem-oriented system of programs for precision spectrometric information processing used in the indicated experiments is described

  18. Joint annual report 1984

    International Nuclear Information System (INIS)

    Hennig, K.

    1985-06-01

    An account is given on the activities in nuclear and solid state physcis. In the field of relativistic nuclear physcis first measurements at the Synchrophasotron of the JINR Dubna are presented. Nuclear reactions with heavy ions have been investigated at the cyclotron U-300 of the JINR. Studies of few-nucleon problems and measurements of fission cross sections at the tandem accelerator at Rossendorf have been continued. High spin states in transition nuclei (A approximately 80) and semimagic nuclei have been studied. Works in nuclear theory comprise heavy ion physics, plasma transitions in hot nuclear matter, antikaon production, hypernuclei and deformed nuclei, the time-dependent Hartree-Fock method, meson exchange, and new aspects of shell models. Various studies in solid state physics are presented, including the following: high-dose implantation in metals and semiconductors, tempering in semiconductor materials, light pulse annealing in Si, neutron diffraction in texture analysis, application of Si in the field of sensor technology

  19. High magnetic field uniformity superconducting magnet for a movable polarized target

    International Nuclear Information System (INIS)

    Anishchenko, N.G.; Bartenev, V.D.; Blinov, N.A.

    1998-01-01

    The superconducting polarizing magnet was constructed for movable polarized target (MPT) with working volume 200 mm long and 30 mm in diameter. The magnet provides a polarizing magnetic field up to 6 T with the uniformity of 4.5 x 10 -4 in the working volume of the target. The magnet windings are made of a NbTi wire, impregnated with the epoxy resin and placed in the horizontal cryostat with 'warm' aperture diameter of 96 mm. The design and technology of the magnet winding are described. Results of the magnetic field map measurements using a NMR-magnetometer are given. The MPT set-up is installed in the beam line of polarized neutrons produced by break-up of polarized deuterons extracted from the Synchrophasotron of the Laboratory of High Energies (LHE), JINR, Dubna

  20. First experiments on transmutation studies of iodine-129 and neptunium-237 using relativistic protons of 3.7 GeV

    International Nuclear Information System (INIS)

    Krivopustov, M.I.; Adam, J.; Bradnova, V.

    1997-01-01

    First experiments on the transmutation of long-lived 129 I and 237 Np using relativistic protons of 3.7 GeV are described. Relativistic protons generate in extended Pb-targets substantial neutron fluences. These neutrons get moderated in paraffin and are used for transmutation as follows: 129 (n, γ) 130 I(β - ) → 130 Xe(stable) and 237 Np(n, γ) 238 Np(β - ) →. The isotopes 130 I (T 1/2 =12.36 h) and 238 Np (T 1/2 =2.117 days) were identified radiochemically. One can estimate the transmutation cross section (n, γ) in the given neutron field as σ( 129 I(n, γ))=(10±2)b and σ( 237 Np(n, γ))=(140±30)b. The experiments were carried out in November 1996 at the Synchrophasotron, Laboratory of High Energies (LHE), Dubna, Russia

  1. Investigation of Neutron Spectra and Transmutation of ^{129}I, ^{237}Np and Other Nuclides with 1.5 GeV Protons from the Dubna Nuclotron Using the Electronuclear Setup "Energy plus Transmutation"

    CERN Document Server

    Krivopustov, M I; Balabekyan, A R; Batusov, Yu A; Bielewicz, M; Brandt, R; Chaloun, P; Chultem, D; Dwivedi, K K; Elishev, A F; Fragopoulou, M; Henzl, V; Henzlová, D; Kalinnikov, V G; Kievets, M K; Krása, A; Krizek, F; Kugler, A; Manolopoulou, Metaxia; Mariin, I I; Nourreddine, A; Odoj, R; Pavliouk, A V; Pronskikh, V S; Robotham, H; Siemon, K; Szuta, M; Stegailov, V I; Solnyshkin, A A; Sosnin, A N; Stoulos, S; Tsoupko-Sitnikov, V M; Tumendelger, T; Wojecehowski, A; Wagner, V; Wan, J S; Westmeier, W; Zamani-Valasiadou, M; Kumawat, H; Kumar, V; Zaverioukha, O S; Zhuk, I V

    2004-01-01

    Experiments which are part of the scientific program "Investigations of physical aspects of electronuclear method of energy production and transmutation for radioactive waste of atomic energetics using relativistic beams from the JINR Synchrophasotron/Nuclotron" (project "Energy plus Transmutation") are described. A large lead target surrounded by a four-section uranium blanket with total weight of 206.4 kg natural uranium was irradiated with 1.5 GeV protons from the new cryogenic accelerator Nuclotron. Radiochemical sensors were exposed to the secondary particle fluences inside and on top of the target assembly. Two long-lived radioactive waste of atomic energetics sensors ^{129}I and ^{237}Np (approximately 1 g weight each) and stable nuclides ^{27}Al, ^{59}Co, ^{127}I, ^{139}La, ^{197}Au and ^{209}Bi as well as natural and enriched uranium were used. In addition, various solid state nuclear track detectors and nuclear emulsions were exposed simultaneously. The experimental results confirm the theoretical e...

  2. Commercial accelerators: Compact superconducting synchrocyclotrons with magnetic field up to 10 T for proton and carbon therapy

    Science.gov (United States)

    Papash, A. I.; Karamysheva, G. A.; Onishchenko, L. M.

    2012-11-01

    Based on a brief review of accelerators widely used for proton-ion therapy and for curing patients over the last 20 years, the necessity and feasibility of creating compact superconducting synchrocyclotrons with a magnetic field value up to 10 T are outlined. The main component of modern commercial facilities for proton-ion therapy is an isochronous cyclotron with room-temperature or superconducting coils which accelerates protons to 250 MeV or a synchrophasotron with carbon-ion energy reaching 400 MeV/nucleon. Usually the ions are delivered from the accelerator to the medical-treatment room via transport lines, while irradiation is produced by means of a system that is comprised of pointing magnets, collimators, and energy degraders mounted on a rotating gantry. To greatly reduce the price of the facility (by an order of magnitude) and to facilitate the work of hospital personnel, the isocentric rotation of a compact superconducting synchrocyclotron around the patient is proposed. Estimates of the physical and technical parameters of the facility are given.

  3. Transmutation of $^{239}$Pu and Other Nuclides Using Spallation Neutrons Produced by Relativistic Protons Reacting with Massive U- and Pb-Targets

    CERN Document Server

    Adam, J; Bamblevski, V P; Barabanov, M Yu; Bradnova, V; Chaloun, P; Hella, K M; Kalinnikov, V G; Krivopustov, M I; Kulakov, B A; Perelygin, V P; Pronskikh, V S; Pavliouk, A V; Solnyshkin, A A; Sosnin, A N; Stegailov, V I; Tsoupko-Sitnikov, V M; Zaverioukha, O S; Adloff, J C; Debeauvais, M; Brandt, R; Langrock, E J; Vater, P; Van, J S; Westmeier, W; Dwivedi, K K; Guo Shi Lun; Li Li Qiang; Hashemi-Nezhad, S R; Kievets, M K; Lomonosova, E M; Zhuk, I V; Modolo, G; Odoj, R; Zamani-Valassiadou, M

    2001-01-01

    Experimental studies on the transmutation of some long-lived radioactive waste nuclei, such as ^{129}I, ^{237}Np, and ^{239}Pu, as well as on natural uranium and lanthanum (all of them used as sensors) were carried out at the Synchrophasotron of the Laboratory for High Energies (JINR, Dubna). Spallation neutrons were produced by relativistic protons with energies in the range of 0.5 GeV\\le E(p)\\le 1.5 GeV interacting with 20 cm long uranium or lead target stacks. The targets were surrounded by 6 cm paraffin moderators. The radioactive sensors mentioned above were positioned on the outside surface of the moderator and contained typically approximately 0.5 up to 1 gram of long-lived isotopes. The highly radioactive targets were produced perfectly well-sealed in aluminum containers by the Institute of Physics and Power Engineering, Obninsk, Russia. From the experimentally observed transmutation rates one can easily extrapolate, that in a subcritical nuclear power assembly (or "energy amplifier") using a 10 mA pr...

  4. First radiochemical studies on the transmutation of 239Pu with spallation neutrons

    International Nuclear Information System (INIS)

    Wan, J.-S.; Langrock, E.-J.; Westmeier, W.

    2000-01-01

    Incineration studies of plutonium were carried out at the synchrophasotron of the Joint Institute for Nuclear Research (Dubna) using proton beams with energies of 0.53 GeV and 1.0 GeV. Solid lead target (8 cm in diameter and 20 cm long) was surrounded with 6 cm thick paraffin as neutron moderator and then irradiated. The transmutation of 239 Pu and the associated production of fission products 91 Sr, 92 Sr, 97 Zr, 99 Mo, 103 Ru, 105 Ru, 129 Sb, 132 Te, 133 I, 135 I and 143 Ce were studied. The plutonium samples (each 449 mg) were placed on the outer surface of moderator. For 1.0 GeV proton beam, the fission rate of 239 Pu is 0.0032 fissions per proton in one gram plutonium samples, for 0.53 GeV proton this value is 0.0022. The experimental uncertainty is about 15%. The experiments are compared to two theoretical model calculations with moderate success, using the Dubna Cascade Model (CEM) and the LAHET code. The practical incineration rate of 239 Pu is very high. For example: if one uses 10mA, 1 GeV proton beams under the same (fictive) experimental conditions, the incineration rate of 239 Pu via fission is 3 mg out of the 449 mg sample per day. For 0.53 GeV protons the corresponding rate is 2 mg per day

  5. Neutron yields from massive lead and uranium targets irradiated with relativistic protons

    International Nuclear Information System (INIS)

    Zamani, M.; Fragopoulou, M.; Stoulos, S.; Manolopoulou, M.; Kulakov, B.A.; Krivopustov, M.I.; Sosnin, N.A.; Brandt, R.; Westmeier, W.; Debeauvais, M.; Hashemi-Nezhad, S.R.

    2005-01-01

    Long-lived isotopes can be transmuted into stable or short-lived elements either by neutron captures or neutron induced fission. The need of a large excess of neutrons has led to the use of accelerator driven sources (ADS). A series of experiments were carried out at the Synchrophasotron/Nuclotron of the Joint Institute for Nuclear Research (JINR) Dubna, using protons of 1.0 GeV. Solid Lead and Uranium targets surrounded by paraffin moderator were irradiated. On the outer surface of the moderator a number of Solid State Track Detectors were placed to monitor neutron spatial distribution. The results showed that the maximum neutron production was reached within the range of one to two proton mean free paths in the target. Then decreasing neutron production follows the proton beam attenuation along the target. Moreover, the results showed both targets neutron production evolution along the target, to be the same. However, neutron flux per incident proton is depended on the target mass, which was found to be higher for the heavier target

  6. Measurement of the total cross section difference Δσ L in np transmission at 1.19, 2.49 and 3.65 GeV

    Science.gov (United States)

    Adiasevich, B. P.; Antonenko, V. G.; Averichev, S. A.; Azhgirey, L. S.; Ball, J.; Bazhanov, N. A.; Benda, B.; Borisov, N. S.; Borzunov, Yu. T.; Bunyatova, E. I.; Burinov, V. F.; Chernykh, E. V.; Dolgii, S. A.; Durand, G.; Dzyubak, A. P.; Fedorov, A. N.; Fimushkin, V. V.; Fontaine, J. M.; Glagolev, V. V.; Golovanov, L. B.; Grosnick, D. P.; Gurevich, G. M.; Hill, D. A.; Karpunin, A. V.; Kasprzyk, T. E.; Khachaturov, B. A.; Kirillov, A. D.; Kochelev, N. I.; Kovalenko, A. D.; Kovalev, A. I.; Kulikov, M. V.; Ladygin, V. P.; Lazarev, A. B.; Lehar, F.; de Lesquen, A.; Liburg, M. Yu.; Lopiano, D.; Lukhanin, A. A.; Maniakov, P. K.; Matafonov, V. N.; Matyushevsky, E. A.; Mgebrishvili, G.; Mironov, S. V.; Neganov, A. B.; Nikolaevsky, G. P.; Nomofilov, A. A.; Pilipenko, Yu. K.; Pisarev, I. L.; Piskunov, N. M.; Plis, Yu. A.; Polunin, Yu. P.; Polyakov, V. V.; Prokofiev, A. N.; Ronzhin, D. A.; Rukoyatkin, P. A.; Sans, J. L.; Sharov, V. I.; Shilov, S. N.; Shishov, Yu. A.; Shutov, V. B.; Sorokin, P. V.; Spinka, H. M.; Starikov, A. Yu.; Stoletov, G. D.; Strokovsky, E. A.; Strunov, L. N.; Svetov, A. L.; Teterin, V. V.; Topalov, S. V.; Trautman, V. Yu.; Tsvinev, A. P.; Usov, Yu. A.; Vikhrov, V. V.; Volkov, V. I.; Yershov, A. A.; Yershov, V. P.; Zaporozhets, S. A.; Zhdanov, A. A.

    1996-03-01

    Results of the total cross section difference Δσ L in a np transmission experiment at 1.19, 2.49 and 3.65 GeV incident neutron beam kinetic energies are presented. Measurements were performed at the Synchrophasotron of the Laboratory of High Energies of the Joint Institute for Nuclear Research in Dubna. Results were obtained with a polarized beam of free quasi-monochromatic neutrons passing through the new Dubna frozen spin proton target. The beam and target polarizations were oriented longitudinally. The present results were obtained at the highest energies of free polarized neutrons that can be reached at present. They extend the energy range of existing results from PSI, LAMPF and Saclay measured between 0.066 and 1.10 GeV. The new results are compared with Δσ L( pn) data determined as a difference between Δσ L( pd) and Δσ L( pp) ANL-ZGS measurements. The values of Δσ L for the isospin state I=0 were deduced using known pp data.

  7. Measurement of the total cross section difference {Delta}{sigma} {sub L} in np transmission at 1.19, 2.49 and 3.65 GeV

    Energy Technology Data Exchange (ETDEWEB)

    Adiasevich, B.P. [Rossijskij Nauchnyj Tsentr ``Kurchatovskij Inst.``, Moscow (Russian Federation); Antonenko, V.G. [Rossijskij Nauchnyj Tsentr ``Kurchatovskij Inst.``, Moscow (Russian Federation); Averichev, S.A. [Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of High Energy; Azhgirey, L.S. [Laboratory of Nuclear Problems, JINR, 141980 Dubna, Moscow Region (Russian Federation); Ball, J. [Laboratoire National SATURNE, CNRS/IN2P3 and CEA/DSM, CE Saclay, F-91191 Gif sur Yvette Cedex (France); Bazhanov, N.A. [Petersburg Nuclear Physics Institute, 188350, Gatchina (Russian Federation); Benda, B. [CEA-DAPNIA, CE Saclay, F-91191 Gif sur Yvette Cedex (France); Borisov, N.S. [Laboratory of Nuclear Problems, JINR, 141980 Dubna, Moscow Region (Russian Federation); Borzunov, Yu.T. [Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of High Energy; Bunyatova, E.I. [Laboratory of Nuclear Problems, JINR, 141980 Dubna, Moscow Region (Russian Federation); Burinov, V.F. [Laboratory of Nuclear Problems, JINR, 141980 Dubna, Moscow Region (Russian Federation); Chernykh, E.V. [Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of High Energy; Dolgii, S.A. [Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of High Energy; Durand, G. [CEA-DAPNIA, CE Saclay, F-91191 Gif sur Yvette Cedex (France); Dzyubak, A.P. [Kharkov Institute of Physics and Technology, Academicheskaya str. 1, 310108 Kharkov (Ukraine); Fedorov, A.N. [Laboratory of Particle Physics, JINR, 141980 Dubna, Moscow Region (Russian Federation); Fimushkin, V.V. [Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of High Energy; Fontaine, J.M. [Laboratoire National SATURNE, CNRS/IN2P3 and CEA/DSM, CE Saclay, F-91191 Gif sur Yvette Cedex (France); Glagolev, V.V. [Joint Inst. for Nuclear Research, Dubna (Russian Federation). Lab. of High Energy; Golovanov, L.B.

    1996-06-01

    Results of the total cross section difference {Delta}{sigma} {sub L} in a np transmission experiment at 1.19, 2.49 and 3.65 GeV incident neutron beam kinetic energies are presented. Measurements were performed at the Synchrophasotron of the Laboratory of High Energies of the Joint Institute for Nuclear Research in Dubna. Results were obtained with a polarized beam of free quasi-monochromatic neutrons passing through the new Dubna frozen spin proton target. The beam and target polarizations were oriented longitudinally. The present results were obtained at the highest energies of free polarized neutrons that can be reached at present. They extend the energy range of existing results from PSI, LAMPF and Saclay measured between 0.066 and 1.10 GeV. The new results are compared with {Delta}{sigma} {sub L} (pn) data determined as a difference between {Delta}{sigma} {sub L} (pd) and {Delta}{sigma} {sub L} (pp) ANL-ZGS measurements. The values of {Delta}{sigma} {sub L} for the isospin state I=0 were deduced using known pp data. (orig.). With 5 figs., 7 tabs.

  8. Superconducting polarizing magnet for a movable polarized target

    International Nuclear Information System (INIS)

    Anishchenko, N.G.; Bartenev, V.D.; Blinov, N.A.

    1998-01-01

    The superconducting polarizing magnet was constructed for the JINR (Dubna) movable polarized target (MPT) with working volume 200 mm long and 30 mm in diameter. The magnet provides a polarizing magnetic field up to 6 T in the centre with the uniformity of 4.5 x 10 -4 in the working volume of the target. The magnet contains a main solenoidal winding 558 mm long and 206/144 mm in diameters, and compensating and correcting winding placed at its ends. The windings are made of a NbTi wire, impregnated with the epoxy resin and placed in the horizontal cryostat. The diameter of the 'warm' aperture of the magnet cryostat is 96 mm. The design and technology of the magnet winding are described. Results of the magnetic field map measurements, using a NMR-magnetometer are given. A similar magnet constructed at DAPNIA, CEA/Saclay (France), represented a model for the present development. The MPT array is installed in the beam line of polarized neutrons produced by break-up of polarized deuterons extracted from the synchrophasotron of the Laboratory of High Energies (LHE), JINR (Dubna)

  9. Transmutation of radioactive waste with the help of relativistic heavy ions

    International Nuclear Information System (INIS)

    Brandt, R.; Wan, J.S.; Ochs, M.

    1997-01-01

    A series of experiments was carried out at the Synchrophasotron, LHE, JINR, Dubna, using 3.67 GeV protons and 18 GeV 12 C ion beams. Two massive lead and uranium targets surrounded by paraffin moderator were irradiated. The outer surface of the moderator was some small U- and La-sensors, to be studied by radiochemistry activation techniques, and also by solid-state nuclear track detectors. Both experimental techniques independently give approximately 28 low energy neutrons on the outer surface of the moderator per 3.67 GeV proton hitting the Pb-target. Theoretical estimations based on LAHET and DCM/CEM computer codes give considerably smaller fluences: approximately 7-9 low energy neutrons ( 129 I(T 1/2 =2.4 days), could be identified radiochemically as well as other spallation products. The transmutation rates are substantial: a 10 mA accelerator of 3.67 GeV protons could transmute at least 30% of 237 Np and 1% of 129 I per month under the given geometrical conditions

  10. Experimental problems of search for quark-gluon plasma in nucleus-nucleus interactions

    International Nuclear Information System (INIS)

    Okonov, Eh.O.

    1987-01-01

    Experimental problems for searching for quark-gluon (quagma) plasma in nucleus-nucleus interactions (NbNb,CaCa, ArPb, CnE, ONe) in the energy range E=0.4-1 GeV/A and 3.67 GeV/A and 200 GeV/A energies are discussed. Peculiarities of performing experiments on Dubna synchrophasotron and SPS Bevalac are discussed. The first results prove hadron matter thermalization sufficient for quagma manifestation. It is found that such characteristics of studied interactions as relative λ-hyperon yield, spectral (temperature) characteristics of λ k -hyperons (with higher values of transferred transverse momenta) and associatively produced peons are of greatest interest. The necessity of precise establishment of λ-hyperon group as excessive and differing in its origin from the other particles of the hadron phase is noted. It is shown that experimental approach used in Dubna research proved efficient and requires further development. It includes : selection of rare events (fluctuations) in central interactions of nuclei with high local excitation; search and research of peculiarities in the production of strange particles and in associative pion production; use of streamer spectrometer with a trigger system of rigid selection of central interactions

  11. DUBNA: Spin effects

    International Nuclear Information System (INIS)

    Anon.

    1995-01-01

    Full text: Earlier this year, a collaboration of Russian, Ukrainian and French laboratories measured the difference between the polarized neutron and proton total reaction rate (total cross section difference) at slightly higher energies than previous experiments, providing an interesting hint of an effect predicted by theory. This was measured using a beam of longitudinally polarized neutrons and a longitudinally polarized proton target with parallel and antiparallel polarization directions. The polarized neutron beam, from the break-up of polarized deuterons, was accelerated by the Synchrophasotron at the Joint Institute for Nuclear Research (JINR) Laboratory of High Energies, Dubna (Russian Federation). The polarized target, 20 cm long and 3 cm in diameter, provided by DAPNIA (Saclay, France) and Argonne (USA), had also been used in 1989-1990 at Fermilab for the E704 experiment. Equipment from Saclay and Argonne was shipped to Dubna and work started in June 1994. The International Association for the Promotion of Cooperation with Scientists from the Independent States of the Former Soviet Union (INTAS) supported the construction and improvement of the target in a suitable transportable form. The target was mounted in the JINR Laboratory of Nuclear Problems (LNP) by experts from DAPNIA (Saclay), JINR Dubna (LNP, LHE and Laboratory of Particle Physics - LPP), Gatchina (Russia), RASMoscow and the Kharkov (Ukraine) laboratories. The Saturne National Laboratory (Saclay), helped with computer programmes for the NMR target polarization measurements. Apparatus was tested in early February. The beam of 2 x 109 polarized deuterons produced 106 polarized neutrons at 3.6 GeV. The neutron beam polarization was about 52%. The new superconducting Nuclotron accelerator should allow the beam intensity to be increased and beam quality improved after an upgrade of the injection system. Preliminary results for the polarized neutron-proton cross section difference at neutron kinetic

  12. Production of alpha-particles in 16Op-interactions at 3.25 A GeV/c

    International Nuclear Information System (INIS)

    Bazarov, E.; Gulamov, K.G.; Lutpullaev, S.L.; Olimov, K.; Yuldashev, A.A.; Glagolev, V.V.; Ismatov, E.I.; Karshiev, D.A.; Khamidov, Kh.Sh.; Yuldashev, B.S.; Fazylov, M.I.

    2004-01-01

    Full text: Given report presents the results of studies of mechanisms of alpha-particles production in 16 Op-interactions at 3.25 A GeV/C. The experimental results were compared with predictions of cascade-fragmentation evaporation model (CFEM). For 16 O light nucleus a contribution of evaporative processes in cross section of fragments production is negligibly small and Fermi break-up is considered to be main fragments production mechanism. The experimental material obtained from HEL JINR 1-meter hydrogen bubble chamber, irradiated by relativistic oxygen-16 nuclei at Dubna synchrophasotron, consisting of more than 11000 16 Op-events. Questions related to processing stereo images from 1-meter hydrogen bubble chamber as well as to the procedure of secondary particles and fragments identification are discussed in details in [2-4]. In work [2] in 12 CEm-interactions at 4.5 A GeV/C the azimuthal asymmetries and colinearities were observed in two and three alpha-particle production channels. This experimental fact as well as disagreement between experimental transverse momentum spectra of alpha-particles and predictions of fragmentation statistical model [3] was qualitatively interpreted within phenomenological model of cylinder phase space with transverse momentum and possible angular moment acquired by 'remnant nucleus' at interaction with target. Therefore, to check an alternative physical picture allowing one to have quantitative explanation we have conducted similar experimental studies, which were compared with the results of corresponding original Monte Carlo calculation of work [1]. The main differences are the following: consideration of energy-momentum conservation laws in every event with relative accuracy of 10 -6 , generation of events in accordance with experimental probabilities of every exclusive (excluding pions) initial nucleus break-up channel, generation of components of momenta transferred to fragmenting nucleus by proton-nucleus in form of Gauss

  13. On the possibility of the geometrical reconstruction of the charged particle trajectories in the streamer chamber

    International Nuclear Information System (INIS)

    Constantin, F.; Jipa, A.; Ilie, Gh.

    1998-01-01

    An interesting problem in the experiments using visualisation detectors is that of the geometrical reconstruction of the trajectories. In this work a new method for the geometrical reconstruction of trajectories of the charged particles produced in nucleus-nucleus collisions at 4.5 A GeV/c is proposed. The experiments have been performed at the JINR Synchrophasotron, in the frame of the SKM 200 Collaboration. The geometrical reconstruction method is based on the facilities offered by the Sun3VME-MaxVideo20 work-station, a real time image processing machine produced by DataCube Corporation. An algorithm is constructed taking into account some relevant characteristics of the pictures. For a typical picture, the centre, a very noisy region, is the starting point for all main tracks (the vertex); the poor contrast makes tracks identification difficult. Surrounding this first region there is an almost circular belt with a better contrast and without overlapping tracks. Finally, the third region, the outer one, is the origin of the secondary tracks, which is also noisy. The secondary tracks identify particles created in the chamber far from the vertex; secondary particle creation induces a large noise into the image and the sharpness reduces. The areas of these three regions vary from one picture to other, their fractions amounting around 20%, 50%, and 30%, respectively. The algorithm treats the primary tracks only. It takes great advantage for the well-defined geometrical vertex position. The primary tracks represent curved trajectories of charged particles moving in a magnetic field. As curved tracks are harder to identify relative to straight lines, we propose a conformal transformation from the surface z = x + iy to the surface w = u + iv related by the relation z a 2 /w. It transforms circles passing through origin in z plane into straight lines in w plane. The a 2 factor is a constant which must be determined. Practically, we transform a discrete image by