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BiBTeX citation export for WEPOPT002: Conception of High Intensive Polarized Proton Beam Formation in NICA Collider

@inproceedings{syresin:ipac2022-wepopt002,
  author       = {E. Syresin and A.V. Butenko and Y. Filatov and S.D. Kolokolchikov and A.M. Kondratenko and M.A. Kondratenko and S.A. Kostromin and O.S. Kozlov and I.N. Meshkov and N.V. Mityanina and Y. Senichev and A.O. Sidorin and G.V. Trubnikov and A. Tuzikov and P.R. Zenkevich},
% author       = {E. Syresin and A.V. Butenko and Y. Filatov and S.D. Kolokolchikov and A.M. Kondratenko and M.A. Kondratenko and others},
% author       = {E. Syresin and others},
  title        = {{Conception of High Intensive Polarized Proton Beam Formation in NICA Collider}},
  booktitle    = {Proc. IPAC'22},
% booktitle    = {Proc. 13th International Particle Accelerator Conference (IPAC'22)},
  pages        = {1822--1824},
  eid          = {WEPOPT002},
  language     = {english},
  keywords     = {proton, collider, injection, luminosity, acceleration},
  venue        = {Bangkok, Thailand},
  series       = {International Particle Accelerator Conference},
  number       = {13},
  publisher    = {JACoW Publishing, Geneva, Switzerland},
  month        = {07},
  year         = {2022},
  issn         = {2673-5490},
  isbn         = {978-3-95450-227-1},
  doi          = {10.18429/JACoW-IPAC2022-WEPOPT002},
  url          = {https://jacow.org/ipac2022/papers/wepopt002.pdf},
  abstract     = {{NICA (Nuclotron-based Ion Collider fAcility) is a new accelerator complex being assembled at JINR to search for the mixed phase of baryonic matter and to investigate the nature of nucleon/particle spin. The polarized proton beams will be operated at the energy range of 5-12.6 GeV, the beam intensity in each ring of 2.2x10¹³ and the luminosity of 1x10³² cm⁻² s⁻¹. The conception of formation of high intensive proton beams is discussed for two different schemes. In first scheme the protons are injected from Nuclotron to Collider at an energy of 2-2.5 GeV to provide the cooling and the storage at this energy and then they are accelerated up to energy of experiments. In the second scheme the cooling of protons is realized in one from accelerators of the injection chain and the protons are injected from Nuclotron to Collider at energy of experiments, where they are stored up required intensity.}},
}