A. B. Neganov
Joint Institute for Nuclear Research
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by A. B. Neganov.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
N. A. Bazhanov; B. Benda; N. S. Borisov; A. P. Dzyubak; G. Durand; L.B. Golovanov; G. M. Gurevich; A. I. Kovalev; A. B. Lazarev; F. Lehar; A. A. Lukhanin; A. B. Neganov; S.V. Topalov; S. Shilov; Yu. A. Usov
A movable polarized target has a volume 140 cm3 (20 cm long and 3 cm diameter). Polarizing magnet was tested to 6.5T, homogeneity is better than 2 × 10−4. The nuclear spin relaxation time in a frozen mode (at a temperature 50 mK and magnetic field 2.5T) is over 1000 h. Maximum values of proton polarization obtained were 80% and 85% for positive and negative polarization, respectively.
Nuclear Physics | 1985
V. D. Apokin; I. A. Avvakumov; N. I. Belikov; Yu. Sh. Bagaturia; N. S. Borisov; A.A. Derevshchikov; L.N. Glonti; Yu. M. Kazarinov; B. A. Khachaturov; M. Yu. Liburg; V. N. Mataphonov; Yu. A. Matulenko; G. Macharashvili; A.P. Meshchanin; A.A. Morozov; A. I. Mysnik; A. B. Neganov; B. S. Neganov; S. B. Nurushev; L. B. Parfenov; A. F. Prudkoglyad; V. L. Rykov; V.V. Siksin; L. F. Soloviev; V.L. Solovianov; Yu. A. Usov; A. N. Vasiliev
Abstract The paper presents results on measuring the polarization in the reaction π − p→ π 0 n at 40 GeV/ c in the 4-momentum transfer range 0 t |⩽2 (GeV/ c ) 2 . The results based on the statistics of about 2.2 million recorded events made it possible to observe a noticeable value and complex structure in the polarization behaviour up to | t |⩽2 (GeV/ c ) 2 .
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1998
N. A. Bazhanov; B. Benda; N. S. Borisov; G. Durand; A. P. Dzyubak; A. N. Fedorov; L.B. Golovanov; G. M. Gurevich; I. Karnaukhov; A. I. Kovalev; A. B. Lazarev; F. Lehar; A. A. Lukhanin; V. N. Matafonov; A. B. Neganov; Yu. A. Plis; S. Shilov; S.V. Topalov; Yu. A. Usov
Experience with polarized targets [1,2] and achieving of very low temperatures in 1966 at the Laboratory of Nuclear Problems [3] and by another group [4] gave rise to the idea of using a radically new technique based on dissolving 3He in 4He to create a frozen spin polarized target. The short history of the development of such proton and deuteron targets at the LNP is given. The complex Cr(V) compounds in diols are used as target operating material. A characteristic feature of these targets is a long relaxation time (∼ 1000h) in magnetic fields of about 0.5 T. Lately, the Saclay-Argonne frozen spin proton polarized target used initially in E704 experiment at FERMILAB has been upgraded with adding the missing parts and the first physics experiment has been carried out.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994
N. S. Borisov; V. N. Matafonov; A. B. Neganov; Yu. A. Plis; O. N. Shchevelev; Yu. A. Usov; I. Jánský; M. Rotter; B. Sedlák; I. Wilhelm; G. M. Gurevich; A. A. Lukhanin; J. Jelínek; A. Srnka; L. Skrbek
Abstract A target with a frozen spin polarization of protons in 1.2-propanediol with a paramagnetic Cr(V) impurity is described, intended for polarization parameter studies in np-scattering at approximately 15 MeV neutron energy. The target of cylindrical shape of 2 cm diameter and 6 cm long with an initial polarization of 95 ± 3%, obtainable by the dynamic polarization technique, is placed at a temperature about 20 mK in a magnetic field of 0.37 T generated by a magnetic system, which provides a large aperture for scattered particles. The relaxation time for the spin polarization in an experiment is about 1000 hours.
Journal of Physics E: Scientific Instruments | 1988
N. S. Borisov; E I Bunyatova; M. Yu. Liburg; V. N. Matafonov; A. B. Neganov; Yu. A. Usov
A frozen spin polarised deuteron target cooled by a dilution refrigerator is described. Fully deuterated ethanediol and propanediol synthesised with a Cr(V) complex are used as the target materials. The following results are obtained: the maximum polarisation is 0.4, the maximum spin-lattice relaxation time is up to approximately 1500 h at 20 mK and 0.53 T.
Journal of Instrumentation | 2010
A. Afonin; A. V. Akimov; T. Barillari; V. Bezzubov; M. Blagov; H. M. Braun; D. Bruncko; Sergey Chekulaev; A. Cheplakov; R. Degele; S. P. Denisov; V. Drobin; P. Eckstein; V. Ershov; V. N. Evdokimov; J. Ferencei; V. Fimushkin; A. Fischer; H. Futterschneider; V. Garkusha; A. Glatte; C. Handel; J. Huber; N. Javadov; M. Y. Kazarinov; A. Khoroshilov; A. E. Kiryunin; E. Kladiva; M. Kobel; A. A. Komar
In this paper it is shown that a measurement of the relative luminosity changes at the LHC may be obtained by analysing the currents drawn from the high voltage power supplies of the electromagnetic section of the forward calorimeter of the ATLAS detector. The method was verified with a reproduction of a small section of the ATLAS forward calorimeter using proton beams of known beam energies and variable intensities at the U-70 accelerator at IHEP in Protvino, Russia. The experimental setup and the data taking during a test beam run in April 2008 are described in detail. A comparison of the measured high voltage currents with reference measurements from beam intensity monitors shows a linear dependence on the beam intensity. The non-linearities are measured to be less than 0.5% combining statistical and systematic uncertainties.
Physics of Particles and Nuclei | 2013
A. Thomas; N. S. Borisov; H. J. Arends; A. N. Fedorov; G. M. Gurevich; R. L. Kondratiev; M. Korolija; A. B. Lazarev; M. Martinez; W. Meyer; S. V. Mironov; A. B. Neganov; V. N. Pavlov; H. Ortega; G. Reicherz; Yu. A. Usov
The new frozen spin polarized target for experiments at the polarized beam of the real photon facility A2 of the MAMI accelerator is described. The A2-collaboration at the Mainz Microtron MAMI is measuring photon absorption cross section using circularly and linearly polarized photons up to the energy of 1.5 GeV. The photons are produced in the’ Bremsstrahlungs’ process. In the years 2005/2006 the Crystal Ball detector with its unique capability to cope with multi photon final states was set up in Mainz. Since 2010 the experimental apparatus has been completed by a polarized target. The horizontal dilution refrigerator of the Frozen-Spin Target has been constructed and is operated in close cooperation with the Joint Institute for Nuclear Research in Dubna, Russia. The system offers the opportunity to provide longitudinally and transversely polarized protons and deuteron. In this paper the operation experience of this new Frozen-Spin Target and first results from the runs in 2010 and 2011 are presented.
Journal of Physics: Conference Series | 2011
V. V. Abramov; N. I. Belikov; Y. Goncharenko; V. N. Grishin; A. M. Davidenko; A.A. Derevshchikov; V. Kachanov; D. A. Konstantinov; V. A. Kormilitsyn; Yu. M. Melnik; A.P. Meshchanin; N. G. Minaev; V. V. Mochalov; D. A. Morozov; L. V. Nogach; S. B. Nurushev; A. V. Ryazantsev; S. V. Ryzhikov; P. A. Semenov; L. F. Soloviev; A. F. Prudkoglyad; A. Uzunian; A. N. Vasiliev; A. E. Yakutin; N. A. Bazhanov; N. S. Borisov; A. B. Lazarev; A. B. Neganov; Yu. A. Plis; O. N. Shchevelev
A new experiment SPASCHARM devoted to a systematic study of polarization phenomena in hadron-hadron interactions in the energy range 10-70 GeV is under preparation at IHEP (Protvino). The physical observables will be single-spin asymmetries, hyperon polarizations and spin-density matrix elements. A universal setup will detect and identify various neutral and charge particles in the full azimuthal angle and a wide polar angle range. A polarized target is used to measure the SSA. The SPASCHARM sub-detectors are being designed and constructed now. The possibility of obtaining a polarized proton beam for the SPASCHARM experiment from Lambda decays is under study.
Physics of Atomic Nuclei | 2010
V. V. Mochalov; N. I. Belikov; N. S. Borisov; A. N. Vasiliev; A. A. Derevschikov; Yu. A. Matulenko; A. P. Meschanin; N. G. Minaev; A. B. Neganov; S. B. Nurushev; A. F. Prudkoglyad; L. F. Soloviev; Yu. A. Usov; A. N. Fedorov; O. N. Schevelev
The single-spin asymmetry AN in the reaction π− + d↑ → π0 + X in the beam-fragmentation region at the energy of 40 GeV was investigated by using the PROZA setup installed at the U-70 accelerator of the Institute for High Energy Physics (IHEP, Protvino). It was measured to be AN = (13.6 ± 2.6(stat.) ± 2.0(syst.))% in the intervals 0.7 < xF < 1.0 and 1.0 < pT < 1.8 GeV/c. The results agree with the asymmetry of π0 mesons in the charge-exchange reaction π− + p↑ → π0 + n at the same values of the transverse momentum and beam energy. The asymmetry in the reaction K− + d↑ → π0 + X was simultaneously measured and found to be AN = (11 ± 14)% for pT > 1.2 GeV/c.
Czechoslovak Journal of Physics | 2005
V.I. Sharov; N. G. Anischenko; V. Antonenko; S.A. Averichev; L. S. Azhgirey; N.A. Bazhanov; A.A. Belyaev; N.A. Blinov; N. S. Borisov; S. B. Borzakov; Yu.T. Borzunov; Yu.P. Bushuev; L.P. Chernenko; E.V. Chernykh; V.F. Chumakov; S. A. Dolgh; A. N. Fedorov; V. V. Fimushkin; Miroslav Finger; M. FingerJr.; L.B. Golovanov; G. M. Gurevich; D.K. Guriev; A. Janata; A.D. Kirillov; E.V. Komogorov; A. D. Kovalenko; A.I. Kovalev; V.A. Krasnov; P. Krstonoshich
New accurate data on the neutron-proton spin-dependent total cross section difference ΔσL(np) at the neutron beam kinetic energies 1.4, 1.7, 1.9 and 2.0 GeV are presented. A number of physical and methodical results on investigation of an elasticnp→pn charge exchange process over a few GeV region are also presented. Measurements were carried out at the Synchrophasotron and Nuclotron of the Veksler and Baldin Laboratory of High Energies of the Joint Institute for Nuclear Research.