Vasily Parkhomchuk
Budker Institute of Nuclear Physics
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PACS2001. Proceedings of the 2001 Particle Accelerator Conference (Cat. No.01CH37268) | 2001
I. Ben-Zvi; Leif A. Ahrens; Michael Brennan; Michael Harrison; Joerg Kewisch; William MacKay; Stephen Peggs; T. Roser; Todd Satogata; Dejan Trbojevic; Vitaly Yakimenko; I. A. Koop; Vasily Parkhomchuk; Vladimir Reva; Yuri Shatunov; Alexander Skrinsky
We introduce plans for electron-cooling of the Relativistic Heavy Ion Collider (RHIC). This project has a number of new features as electron coolers go: It will cool 100 GeV/nucleon ions with 50 MeV electrons; it will be the first attempt to cool a collider at storage-energy; and it will be the first cooler to use a bunched beam and a linear accelerator as the electron source. The linac will be superconducting with energy recovery. The electron source will be based on a photocathode gun. The project is carried out by the Collider-Accelerator Department at BNL in collaboration with the Budker Institute of Nuclear Physics.
Proceedings of the 2005 Particle Accelerator Conference | 2005
I. Ben-Zvi; Vladimir N. Litvinenko; D. Barton; D. Beavis; M. Blaskiewicz; Joseph Brennan; A. Burrill; R. Calaga; P. Cameron; Xiangyun Chang; R. Connolly; Y. Eidelman; A. Fedotov; W. Fischer; D. Gassner; H. Hahn; M. Harrison; A. Hershcovitch; H.-C. Hseuh; A. Jain; P. Johnson; D. Kayran; J. Kewisch; R. Lambiase; W. W. MacKay; G. Mahler; N. Malitsky; G. McIntyre; W. Meng; K.A.M. Mirabella
We report progress on the R&D program for electron-cooling of the Relativistic Heavy Ion Collider (RHIC). This electron cooler is designed to cool 100 GeV/nucleon at storage energy using 54 MeV electrons. The electron source will be a superconducting RF photocathode gun. The accelerator will be a superconducting energy recovery linac. The frequency of the accelerator is set at 703.75 MHz. The maximum electron bunch frequency is 9.38 MHz, with bunch charge of 20 nC. The R&D program has the following components: The photoinjector and its photocathode, the superconducting linac cavity, start-to-end beam dynamics with magnetized electrons, electron cooling calculations including benchmarking experiments and development of a large superconducting solenoid. The photoinjector and linac cavity are being incorporated into an energy recovery linac aimed at demonstrating ampere class current at about 20 MeV.
BEAM COOLING AND RELATED TOPICS: International Workshop on Beam Cooling and Related Topics - COOL05 | 2006
E. Behtenev; V. Bocharov; V. Bubley; M. Vedenev; R. Voskoboinikov; A. Goncharov; Yu. Evtushenko; N. Zapiatkin; M. Zakhvatkin; A. Ivanov; V. Kokoulin; M. Kondaurov; S. Konstantinov; G.S. Krainov; V. Kozak; A. Kruchkov; E.A. Kuper; A. S. Medvedko; L. A. Mironenko; V. Panasiuk; Vasily Parkhomchuk; Vladimir Reva; A. Skrinsky; B. Smirnov; Boris Skarbo; B.N Sukhina; K. Shrainer; X.D. Yang; Hengyu Zhao; J. Li
HIRFL-CSR, a new ion accelerator complex, is under construction at IMP, Lanzhou, China. It is equipped with two electron cooling devices. This article describes the commissioning of cooler at electron energy 300 keV. The cooler is one of the new coolers with some unique manufactured in BINP, Russia. It has a new electron gun producing a hollow electron beam, electrostatic bending and a new structure of solenoid coils at the cooling section. The test results of cooler obtained in Novosibirsk and Lanzhou are reported.
ieee particle accelerator conference | 2007
I. Ben-Zvi; J. Alduino; D. Barton; D. Beavis; M. Blaskiewicz; J.M. Brennan; A. Burrill; R. Calaga; P. Cameron; Xiangyun Chang; A. Drees; A. Fedotov; W. Fischer; G. Ganetis; D. Gassner; J. Grimes; H. Hahn; Lee Hammons; A. Hershcovitch; H.C. Hseuh; D. Kayran; J. Kewisch; R. Lambiase; D. Lederle; Vladimir N. Litvinenko; C. Longo; W. W. MacKay; G. Mahler; G. Mclntyre; W. Meng
The physics interest in a luminosity upgrade of RHIC requires the development of a cooling-frontier facility. Detailed calculations were made of electron cooling of the stored RHIC beams. This has been followed by beam dynamics simulations to establish the feasibility of creating the necessary electron beam. The electron beam accelerator will be a superconducting Energy Recovery Linac (ERL). An intensive experimental R&D program engages the various elements of the accelerator, as described by 24 contributions to the 2007 PAC.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
M. Steck; L Groening; K Blasche; B. Franczak; B. Franzke; T. Winkler; Vasily Parkhomchuk
An electron cooling system has started operation in the heavy ion synchrotron SIS which is used to increase the intensity for highly charged ions. Fast transverse cooling of the hot ion beam after horizontal multiturn injection allows beam accumulation at the injection energy. After optimization of the accumulation process an intensity increase in a synchrotron pulse by more than one order of magnitude has been achieved. For highly charged ions the maximum number of particles has been increased from 1]108 to 1]109. For lighter ions intensity limitations have been encountered which are caused by the high phase space density of the cooled ion beam. Momentum spreads in the 10~4 range and emittances well below 10 p mm mrad have been demonstrated. Recombination losses both in the residual gas and with the free cooler electrons determine the maximum intensity for highly charged ions. Systematic measurements of the recombination rates have been performed providing data for an optimum choice of the charge state. Strong enhancement of the recombination rate with free electrons compared to theoretical calculations of radiative electron capture have been observed. ( 2000 Elsevier Science B.V. All rights reserved.
BEAM COOLING AND RELATED TOPICS: International Workshop on Beam Cooling and Related Topics - COOL05 | 2006
Xiaodong Yang; Vasily Parkhomchuk; Wenlong Zhan; Jiawen Xia; Hongwei Zhao; Youjin Yuan; Mingtao Song; Jie Li; L.J. Mao; Wang Lu; Zhixue Wang
The brief achievements of HIRFL‐CSR commissioning and the achieved parameters of its coolers were presented. With the help of electron cooling code, the cooling time of ion beam were extensive simulated in various parameters of the ion beam in the HIRFL‐CSR electron cooling storage rings respectively, such as ion beam energy, initial transverse emittance, and momentum spread. The influence of the machine lattice parameters‐betatron function, and dispersion function on the cooling time was investigated. The parameters of electron beam and cooling devices were taken into account, such as effective cooling length, magnetic field strength and its parallelism in cooling section, electron beam size and density. As a result, the lattice parameters of HIRFL‐CSR were optimal for electron cooling, and the parameters of electron beam can be optimized according to the parameters of heavy ion beam.
BEAM COOLING AND RELATED TOPICS: International Workshop on Beam Cooling and Related Topics - COOL05 | 2006
Valentin Bocharov; Alexander Bubley; S. Konstantinov; V.M. Panasyuk; Vasily Parkhomchuk
Description of equipment developed at BINP SB RAS for precision solenoid magnetic field measurement is presented in the paper. Transversal field components are measured by small compass‐based sensor during its motion along the field line. The sensor sensitivity is a few tenth parts of mG and is limited in this range by external noise sources only. Scope of the device application is illustrated by results obtained at BINP during tests of cooling solenoids for electron coolers built at the Institute recently.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997
L. Tecchio; G. Bisoffi; Giuseppe Ciullo; A Dainelli; S. Gustafsson; M. F. Moisio; A. Pisent; M. Poggi; B. Yang; A. Burov; N.S. Dikansky; D.V. Pestrikov; Vasily Parkhomchuk; R. Calabrese; V. Guidi; P. Lenisa; T. Clauser; G. Lamanna; M. Rutigliano; V. Stagno; V. Variale; G Di Massa; M.R. Masullo; V. G. Vaccaro; Carmela Marinelli; Emilio Mariotti; L. Moi
Abstract The possibility of generating crystallized ion beams, i.e. beams whose particles are located at fixed positions, has always excited the interest of most people working on particle accelerators. The reason of this interest has many aspects: knowledge either of a completely new research field or of some of the applicative potentialities, connected with crystalline beams, would justify a careful investigation of this subject. After the successful exploitation of electron cooling in several heavy ion storage rings the possibility of generating crystalline ion beams became more realistic. New cooling methods, like laser cooling, give a further opportunity to reach an ultracold system of particles necessary for the state transition to the crystalline configuration. The conceptual design of a low-energy heavy-ion storage ring, called CRYSTAL, proposed for the experimental demonstration of crystalline beams at Legnaro Laboratories is presented. The physics of crystalline beams as well as the main criteria to design a storage ring suitable to crystallize ion beams are discussed. The effects of instabilities for space charge dominated beams, shear forces in dipole magnets and lattice periodicity breaking are also discussed in detail.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995
V.M. Barbashin; S.N. Chumakov; G. Ciullo; N.S. Dikansky; G. Lamanna; P. Lenisa; Vasily Parkhomchuk; A.N. Sharapa; A.V. Shemyakin; L. Tecchio
Abstract The technical solution of a prototype of an electron cooling device without bending magnets is presented. The electron beam with a current of up to 1 A is formed in a “hollow” gun, accelerated up to 20 kV and its energy is recovered in a “hollow” collector with a current loss of less than 10 −4 . Preliminary beam quality tests are described.
Chinese Physics C | 2013
Ma Xinwen; Vasily Parkhomchuk; Yang Xiaodong; V. B. Reva; Li Jie; Mao Li-Jun; Ma Xiao-Ming; Yan Tai-Lai; Xia Jia-Wen; Yuan You-Jin; Xu Hu-Shan; Yang Jian-Cheng; Xiao Guo-Qing
A storage ring equipped with an electron cooler is an ideal platform for dielectronic recombination (DR) experiments. In order to fulfill the requirement of DR measurements at the main Cooler Storage Ring, a detuning system for the precision control of the relative energy between the ion beam and the electron beam has been installed on the electron cooler device. The test run using 7.0 MeV/u C6+ beam was performed with recording the Schottky spectra and the ion beam currents. The influence of pulse heights and widths of the detuning voltage on the ion beam was analyzed. For the small pulse height, the experimental results from the Schottky spectra were in good agreement with the theoretical results. The frequency shift in the Schottky spectra was significantly reduced for the short pulse width. For the large pulse height, an oscillation phenomenon was observed and some effective ways to reduce the oscillation were pointed out. The detailed description of the phenomenon and the theoretical model based on the plasma oscillation is discussed in this paper. The overall results show that the new detuning system works properly, and could fulfill the requirements of future DR experiments.