Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics

Present worldwide (and European) developments and requirements in nuclear physics, related in particular to
 nuclear power needs, call for the development of a new generation of accelerators for the realization of this research. We propose
 to construct a facility at NSC KIPT, which...

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Опубліковано в: :Вопросы атомной науки и техники
Дата:2004
Автори: Dovbnya, A.N., Guk, I.S., Kononenko, S.G., van der Wiel, M., Botman, J.I.M., Tarasenko, A.S.
Формат: Стаття
Мова:Англійська
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2004
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Цитувати:Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics / A.N. Dovbnya, I.S. Guk, S.G. Kononenko, M. van der Wiel, J.I.M. Botman,
 A.S. Tarasenko // Вопросы атомной науки и техники. — 2004. — № 1. — С. 16-18. — Бібліогр.: 14 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
_version_ 1860019005639622656
author Dovbnya, A.N.
Guk, I.S.
Kononenko, S.G.
van der Wiel, M.
Botman, J.I.M.
Tarasenko, A.S.
author_facet Dovbnya, A.N.
Guk, I.S.
Kononenko, S.G.
van der Wiel, M.
Botman, J.I.M.
Tarasenko, A.S.
citation_txt Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics / A.N. Dovbnya, I.S. Guk, S.G. Kononenko, M. van der Wiel, J.I.M. Botman,
 A.S. Tarasenko // Вопросы атомной науки и техники. — 2004. — № 1. — С. 16-18. — Бібліогр.: 14 назв. — англ.
collection DSpace DC
container_title Вопросы атомной науки и техники
description Present worldwide (and European) developments and requirements in nuclear physics, related in particular to
 nuclear power needs, call for the development of a new generation of accelerators for the realization of this research. We propose
 to construct a facility at NSC KIPT, which produces continuous electron beams in the energy range of 5 to 400 MeV with a current up to one hundred microamperes. This facility is foreseen to provide both un-polarized and polarized electron beams of
 small emittance.
 World trends in accelerator developments indicate that the NCS KIPT accelerator should be a superconducting linear accelerator working in continuous mode, or an accelerator with beam recirculation. In both cases it is most expedient to use accelerating
 structures of the TESLA type.
 Estimations of capital expenses and operational costs for construction and operation of either the linear accelerator or the recirculator accelerator point to significant advantages of the second option. An advantage of the recirculator accelerator is also the opportunity to increase the energy in steps, according to the availability of financial means.
 Simulations of the particle movement in the recirculator accelerator, have shown that the output beam parameters satisfy all modern requirements on electron beams, as specified by the research that will be carried out using this facility. Пропонується створити в ННЦ ХФТI установку для одержання безперервних пучків електронів в діапазоні
 енергій 5…400 МеВ зі струмом до декількох сотень мікроамперів з використанням надпровідної прискорювальної
 структури TESLA. В установці будуть одержані як звичайні, так і поляризовані пучки електронів з малим еміттансом. Предлагается создать в ННЦ ХФТИ установку для получения непрерывных пучков электронов в диапазоне энергий 5…400 МэВ с током до нескольких сотен микроампер с использованием сверхпроводящей ускоряющей структуры
 TESLA. На установке предполагается получать как обычные, так и поляризованные пучки электронов с малым эмиттансом.
first_indexed 2025-12-07T16:46:28Z
format Article
fulltext CHOICE OF THE BASIC VARIANT FOR THE NSC KIPT ACCELERATOR ON NUCLEAR AND HIGH ENERGY PHYSICS A.N. Dovbnya1, I.S. Guk1, S.G. Kononenko1, M. van der Wiel2, J.I.M. Botman2, A.S. Tarasenko1 1National Science Center “Kharkov Institute of Physics and Technology”, 1, Academicheskaya st., 61108, Kharkov, Ukraine; E-mail: guk@kipt.kharkov.ua; 2Technische Universiteit Eindhoven, Den Dolech 2, P.O. Box 513, 5600 MB Eindhoven, The Netherlands; E-mail: j.i.m.botman@tue.nl Present worldwide (and European) developments and requirements in nuclear physics, related in particular to nuclear power needs, call for the development of a new generation of accelerators for the realization of this research. We propose to construct a facility at NSC KIPT, which produces continuous electron beams in the energy range of 5 to 400 MeV with a cur- rent up to one hundred microamperes. This facility is foreseen to provide both un-polarized and polarized electron beams of small emittance. World trends in accelerator developments indicate that the NCS KIPT accelerator should be a superconducting linear acceler- ator working in continuous mode, or an accelerator with beam recirculation. In both cases it is most expedient to use accelerating structures of the TESLA type. Estimations of capital expenses and operational costs for construction and operation of either the linear accelerator or the recircu- lator accelerator point to significant advantages of the second option. An advantage of the recirculator accelerator is also the op- portunity to increase the energy in steps, according to the availability of financial means. Simulations of the particle movement in the recirculator accelerator, have shown that the output beam parameters satisfy all mod- ern requirements on electron beams, as specified by the research that will be carried out using this facility. PACS: 29.17.+w 1. INTRODUCTION In the first 80 years of accelerator development the majority of constructed electron linear accelerators and synchrotrons in the energy range of 100…2000 MeV has exhausted the opportunities of their use in nuclear physics because of the small pulse duration with respect to the pulse repetition period. The second life for these accelerators was promised by the use of beam stretchers. About 15 projects of such installations have been proposed. By 2002 only six projects were realized. At present, two of the installations in operation have stopped and have been disassembled; the nuclear physics research is going on only at three installations [1-3]. During the last ten years basically recirculators have been used for experiments with electrons. These were created using acceleration technology on the basis of superconductivity, and also using warm accelerating systems. The extraction of electrons from these facili- ties, in comparison with stretchers, does not represent essential difficulties: JLab, MAMI, S-DALINAC [4-6]. The last achievements in the high technology fabri- cation of accelerating structures for TESLA [7] allow to obtain an accelerating gradient near 35 MeV/m. Use of this structure for operation in a continuous wave (CW) mode allows to design a sufficiently compact accelera- tor with an energy of about 400 MeV, with a continuous beam and with the appropriate parameters for nuclear physics research. The same mode of operations using an injector with very short bunches allows to create either a free electron laser with high brightness or a neutron source with unique characteristics. Already projects using accelerating structures of the TESLA-type in CW mode for free electron lasers in the x-ray range of wavelengths have appeared [8.9]. The first turn of the 40 MeV superconducting linear acceler- ator ELBE is realized [10]. It is intended for use in nu- clear spectroscopy, radiation physics, neutron physics and as the free electron laser in the infra-red area of the spectrum. The linear accelerators LU-2000 and LU-300, con- structed at KIPT in the sixties of the last century, have become outdated and do not answer the requirements of modern physical experiments. A new particle accelera- tor installation with 400 MeV electron energy is pro- posed at NSC KIPT on the basis of available capital structures, using the newest technological achievements in the field of acceleration of electron beams. (If a man- agement of the tendencies in development modern ac- celerator base for reception of continuous electron beams,??) On the basis of modern accelerator develop- ments regarding continuous electron beams, this instal- lation should be either a superconducting linear acceler- ator working in CW mode, or a recirculator on the basis of TESLA-type superconducting accelerating structures. Estimations of costs and other characteristics of the proposed accelerator are based on information about the accelerators in the BESSY SASE-FEL [8] and TESLA [11] projects, using the same structure. ___________________________________________________________ PROBLEMS OF ATOMIC SIENCE AND TECHNOLOGY. 2004. № 1. 16 Series: Nuclear Physics Investigations (42), p. 16-18. mailto:guk@kipt.kharkov.ua 2. 400 MeV SUPERCONDUCTING ELECTRON LINAC Most suitable for accommodation of the linear accel- erator is the lens corridor and target hall at NSC KIPT (see fig.1). This is because these areas adjoin the SP- 103 hall where the magnetic spectrometer is located, and also building 46, which can be used for accommo- dation of the control of theaccelerator complex, and for equipment necessary for physics research on the beams (for beam dynamics research or for research making use of the electron beams?). The SP-103 hall can be used both for accommodation of new spectrometers, and for free electron lasers activities. For obtaining 400 MeV energy using a quite achiev- able gradient of 15…20 MeV/m about 20 standard ac- celerating structures have to be used. For obtaining the necessary final energy, two modules of the TESLA ac- celerating structures are sufficient, as one module con- sists of 12 units with a total length of 15.927 m [11] (???). Fig. 1. Experimental setup at LU-2000 output The minimum rf-gun length with 25 MeV pre-accel- erator would be about 4 m. In this way, the minimum building length for housing the accelerator should be 36 m, so that with additional hardware it must be no shorter than 40 m. For this reason, there are two options for housing the accelerator: in the lens hall and in the target hall with displacement of the accelerator axis relative to the existing beam pathway. The latter is necessary in or- der to place a part of the accelerator in the re-loading tunnel, since the length of the target hall is smaller than needed. The existing re-loading does not permit to place a module of 16 m long in the bunker, however, if one lengthens the existing hatchway by 12 m, this problem should be solved. A study of the positioning of the pro- posed TESLA accelerator in the tunnel indicates that the transverse cross-section of the considered premises can accommodate the accelerator. The cost of one TESLA accelerating structure in the accelerator together with the infrastructure required to run this system (power, vacuum, cryogenic, high-fre- quency, control, etc.), as follows from the assessment of other references [8,11,12], by mass manufacture amounts to 100-215 thousand euro. From budget costs of the TESLA accelerator, based on expenses for the construction of TTF, it follows, that the capital expenses for purchase of the main accelerat- ing modules and RF system of the TESLA accelerator make 51% of all capital expenses, and the cost of annual operation of the accelerator, i.e. expenses for the electric power, regular klystron replacement or restoration, heli- um loss under working condition of the accelerator of 5000 hours per one year make 7% of these expenses. The capital expenses for the 400 MeV linear acceler- ator will amount to more than 6 million euro, and annu- al operational charges - 420 thousand euro. The beam power of such an accelerator will be about 40 KW. The power of cryogenic losses is more than 630 W at a tem- perature of 2K. Yet, power expenses on the cryogenic system will be dominant, and for this reason the total power used by the accelerator will exceed 2.5 MW. 3. 400 MeV RECIRCULATOR WITH SUPER- CONDUCTING ACCELERATING STRUC- TURE Accelerating structures costs of the linear accelerator form the largest part of the common capital expenses of the construction of the installation. Using a beam circu- lation scheme allows to reduce length, and, hence, cost of the accelerating system. Let us consider a 400 MeV recirculator, using the mag- netic equipment from the EUTERPE electron ring [13]. The recirculator is supposed to be placed in the LU- 2000 target hall and beam extraction is to be in SP-103 hall (see fig.2). As the accelerating system is placed in the straight sections of the recirculator, two TESLA structures are supposed to be used in which the beam receives a 36 MeV gain of energy. The recirculator magnetic structure is considered in ref. [14]. At a beam power of the accelerator of 40 kW, the capacity of recirculator magnetic system will not exceed 170 kW. The capacity of the refrigerator should make about 280 kW. Costruction cost of the recirculator mag- netic system is estimated at 280 thousand euro. ___________________________________________________________ PROBLEMS OF ATOMIC SIENCE AND TECHNOLOGY. 2004. № 1. Series: Nuclear Physics Investigations (42), p. 17 4. CONCLUSIONS The comparison of two variants of installation shows essential recirculator advantages, lower capital expenses for the construction of the accelerator, and smaller ex- penses for operation. Use the of the recirculation circuit version of the beam allows consistently increasing the maximal energy in the installation in the process of increasing volume of means found for the realization of the project, creating . Fig.2. Recirculator layout in the LU-2000 target hall on each stage an opportunity for realizing experiments with the beam. So, with the presence of the 10 MeV in- jector and the first distributing magnet, the beam can be guided to the SP-103 hall and to the lens corridor. After installation of the first accelerating module of 36 MeV in the straight sections of the recirculator the opportuni- ty of working with a beam up to 46 MeV in the SP-103 hall will appear. After installation of all four distributing magnets it is possible to work with the beam with this energy in the overload hall and lens corridor. The instal- lation of the accelerating module in other straight sec- tions will allow lifting the beam energy in these work- stations up to 83 MeV. The installation of magnetic ele- ments of the EUTERPE-ring will allow receiving 192 MeV energy in the SP-103 hall and 228 MeV in the overload and lens halls. The complete installation of 5 arcs with 4 magnets in every arc will allow getting 410 MeV energy in SP-103 hall and a little bit lower energy in other halls. The injector replacement will allow effectively to use the accelerator for nuclear physics, as free electron laser and as a neutrons source. REFERENCES 1. K.D. Jacobs, F. Casagrande, M. Farkhondeh, B.G. McAllister, L.W. O'Brien, C. Tschalaer, E. Tsentalovich, F. Wang, G.T. Zwart (MIT-Bates Linear Accelerator Center) Operational Experience with Resonantly Extracted Beams// Proceedings of PAC 2001, Chicago. 2001, p.2587-2589. 2. Linac and ring project, Project report, part a, part b, Lund 2000. 3. http://www-elsa.physik.uni-bonn.de 4. S. Kostial and others, Operation of the S- DALINAC, Related topics and developments //Proceedings of EPAC 2000, Vienna, Austria, p.1759-1761. 5. M.A.D. Wilson. CW Racetrack Microtrons// Pro- ceedings of the PAC 1999. 1999, p. 71-75. 6. http://www.jlab.org 7. TESLA Collaboration Meeting at INFN-LNF Frascati, 26th-28th May 2003. 8. The BESSY SASE-FEL in Berlin-Adlershof. Sec- tionI,http://www.bessy.de/publications/01.felscien- tific/files/4_sc_section1.pdf 9. Study for a proposed Phase 1 Energy Recovery Linac (ERL) Synchrotron Light Source at Cornell University, CHESS Technical Memo 01-003, JLAB-ACT-01-04, 4 July 2001. 10. P. Michel, A. Buchner, P. Evtushenko, F. Gabriel, U. Lehnert, J. Teichert and J. Voigl, Comissioning Of The Elbe Superconducting Electron Linac, //Proceedings of EPAC 2002, Paris, France, р. 817- 819. 11. PART II. The Accelerator. Editors: R. Brinkmann, K. Flöttmann, J. Roßbach, P. Schmösser, N. Walk- er, H. Weise. TESLA Technical Design Report. March 2001. 12. Ady Hershcovitch. TESLA Accelerator Structure. January, 18, 2002 Meeting. BNL, 21.01. 2002. 13. Boling Xi, J.I.M. Botman, C.J. Timmermans, H.L. Hagedoorn. Design study of storage ring EU- TERРE // Nucl. Instr. and Meth. 1992, v. B68, p.101. 14. A.N. Dovbnya, I.S. Guk, S.G. Kononenko, F.A.Peev, M. van der Wiel, J.I.M. Botman, A.S. Tarasenko Magnetic structure of the NSC KIPT nuclear-and-high-energy-physics electron accelerator at 400 MeV (report on this conference). ВЫБОР ВАРИАНТА БАЗОВОЙ УСКОРИТЕЛЬНОЙ УСТАНОВКИ ННЦ ХФТИ ПО ЯДЕРНОЙ ФИ- ЗИКЕ И ФИЗИКЕ ВЫСОКИХ ЭНЕРГИЙ ___________________________________________________________ PROBLEMS OF ATOMIC SIENCE AND TECHNOLOGY. 2004. № 1. Series: Nuclear Physics Investigations (42), p. 18 http://www.bessy.de/publications/01.felscientific/files/4_sc_section1.pdf http://www.bessy.de/publications/01.felscientific/files/4_sc_section1.pdf http://www.lnf.infn.it/ http://www.infn.it/ http://tesla.desy.de/ http://www.jlab.org/ http://www-elsa.physik.uni-bonn.de/ А.Н. Довбня, И.С. Гук, С.Г. Кононенко, M. van der Wiel, J.I.M. Botman, А.С. Тарасенко Предлагается создать в ННЦ ХФТИ установку для получения непрерывных пучков электронов в диапазоне энер- гий 5…400 МэВ с током до нескольких сотен микроампер с использованием сверхпроводящей ускоряющей структуры TESLA. На установке предполагается получать как обычные, так и поляризованные пучки электронов с малым эмиттан- сом. ВИБІР ВАРІАНТА БАЗОВОЇ ПРИСКОРЮВАЛЬНОЇ УСТАНОВКИ ННЦ ХФТІ ПО ЯДЕРНОЇ ФІЗИКИ ТА ФІЗИКИ ВИСОКИХ ЕНЕРГІЙ А.М. Довбня, І.С. Гук, С.Г. Кононенко, M. van der Wiel, J.I.M. Botman, О.С. Тарасенко Пропонується створити в ННЦ ХФТI установку для одержання безперервних пучків електронів в діапазоні енергій 5…400 МеВ зі струмом до декількох сотень мікроамперів з використанням надпровідної прискорювальної структури TESLA. В установці будуть одержані як звичайні, так і поляризовані пучки електронів з малим еміттансом. ___________________________________________________________ PROBLEMS OF ATOMIC SIENCE AND TECHNOLOGY. 2004. № 1. Series: Nuclear Physics Investigations (42), p. 19 E-mail: guk@kipt.kharkov.ua; Den Dolech 2, P.O. Box 513, 5600 MB Eindhoven, The Netherlands; E-mail: j.i.m.botman@tue.nl PACS: 29.17.+w А.Н. Довбня, И.С. Гук, С.Г. Кононенко, M. van der Wiel, J.I.M. Botman, А.С. Тарасенко А.М. Довбня, І.С. Гук, С.Г. Кононенко, M. van der Wiel, J.I.M. Botman, О.С. Тарасенко
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language English
last_indexed 2025-12-07T16:46:28Z
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spelling Dovbnya, A.N.
Guk, I.S.
Kononenko, S.G.
van der Wiel, M.
Botman, J.I.M.
Tarasenko, A.S.
2015-03-18T13:55:37Z
2015-03-18T13:55:37Z
2004
Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics / A.N. Dovbnya, I.S. Guk, S.G. Kononenko, M. van der Wiel, J.I.M. Botman,
 A.S. Tarasenko // Вопросы атомной науки и техники. — 2004. — № 1. — С. 16-18. — Бібліогр.: 14 назв. — англ.
1562-6016
PACS: 29.17.+w
https://nasplib.isofts.kiev.ua/handle/123456789/78474
Present worldwide (and European) developments and requirements in nuclear physics, related in particular to
 nuclear power needs, call for the development of a new generation of accelerators for the realization of this research. We propose
 to construct a facility at NSC KIPT, which produces continuous electron beams in the energy range of 5 to 400 MeV with a current up to one hundred microamperes. This facility is foreseen to provide both un-polarized and polarized electron beams of
 small emittance.
 World trends in accelerator developments indicate that the NCS KIPT accelerator should be a superconducting linear accelerator working in continuous mode, or an accelerator with beam recirculation. In both cases it is most expedient to use accelerating
 structures of the TESLA type.
 Estimations of capital expenses and operational costs for construction and operation of either the linear accelerator or the recirculator accelerator point to significant advantages of the second option. An advantage of the recirculator accelerator is also the opportunity to increase the energy in steps, according to the availability of financial means.
 Simulations of the particle movement in the recirculator accelerator, have shown that the output beam parameters satisfy all modern requirements on electron beams, as specified by the research that will be carried out using this facility.
Пропонується створити в ННЦ ХФТI установку для одержання безперервних пучків електронів в діапазоні
 енергій 5…400 МеВ зі струмом до декількох сотень мікроамперів з використанням надпровідної прискорювальної
 структури TESLA. В установці будуть одержані як звичайні, так і поляризовані пучки електронів з малим еміттансом.
Предлагается создать в ННЦ ХФТИ установку для получения непрерывных пучков электронов в диапазоне энергий 5…400 МэВ с током до нескольких сотен микроампер с использованием сверхпроводящей ускоряющей структуры
 TESLA. На установке предполагается получать как обычные, так и поляризованные пучки электронов с малым эмиттансом.
en
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
Вопросы атомной науки и техники
Состояние действующих и проекты новых ускорителей
Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics
Вибір варіанта базової прискорювальної установки ННЦ ХФТІ по ядерної фізики та фізики високих енергій
Выбор варианта базовой ускорительной установки ННЦ ХФТИ по ядерной фи- зике и физике высоких энергий
Article
published earlier
spellingShingle Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics
Dovbnya, A.N.
Guk, I.S.
Kononenko, S.G.
van der Wiel, M.
Botman, J.I.M.
Tarasenko, A.S.
Состояние действующих и проекты новых ускорителей
title Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics
title_alt Вибір варіанта базової прискорювальної установки ННЦ ХФТІ по ядерної фізики та фізики високих енергій
Выбор варианта базовой ускорительной установки ННЦ ХФТИ по ядерной фи- зике и физике высоких энергий
title_full Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics
title_fullStr Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics
title_full_unstemmed Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics
title_short Choice of the basic variant for the NSC KIPT accelerator on nuclear and high energy physics
title_sort choice of the basic variant for the nsc kipt accelerator on nuclear and high energy physics
topic Состояние действующих и проекты новых ускорителей
topic_facet Состояние действующих и проекты новых ускорителей
url https://nasplib.isofts.kiev.ua/handle/123456789/78474
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AT kononenkosg vyborvariantabazovoiuskoritelʹnoiustanovkinnchftipoâdernoifizikeifizikevysokihénergii
AT vanderwielm vyborvariantabazovoiuskoritelʹnoiustanovkinnchftipoâdernoifizikeifizikevysokihénergii
AT botmanjim vyborvariantabazovoiuskoritelʹnoiustanovkinnchftipoâdernoifizikeifizikevysokihénergii
AT tarasenkoas vyborvariantabazovoiuskoritelʹnoiustanovkinnchftipoâdernoifizikeifizikevysokihénergii