The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis
The СС1-3 cyclotron system is intended to be installed in the laboratory of nuclear-physical methods of the element analysis of the Vinca Institute of Nuclear Sciences, Belgrade, Serbia. The cyclotron system ensures production of a beam of protons with energy in the range from 1 to 3 MeV with a spec...
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| Zitieren: | The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis / O.L. Veresov, Yu.N. Gavrish, A.V. Galchuck, S.V. Grigorenko, V.I. Grigoriev, M.A. Emelianov, L.E. Korolev, A.N. Kuzhlev, I.I. Mezhov, V.G. Mudrolyubov, A.P. Strokach, S.S. Tsygankov, V.D. Shiltsev // Вопросы атомной науки и техники. — 2013. — № 6. — С. 13-15. — англ. |
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nasplib_isofts_kiev_ua-123456789-1118092025-02-09T23:20:32Z The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis Циклотронний комплекс СС1-3 для неруйнівних ядерно-фізичних методів елементного аналізу Циклотронный комплекс СС1-3 для неразрушающих ядерно-физических методов элементного анализа Veresov, O.L. Gavrish, Yu.N. Galchuck, A.V. Grigorenko, S.V. Grigoriev, V.I. Emelianov, M.A. Korolev, L.E. Kuzhlev, A.N. Mezhov, I.I. Mudrolyubov, V.G. Strokach, A.P. Tsygankov, S.S. Shiltsev, V.D. Состояние действующих и проекты новых ускорителей The СС1-3 cyclotron system is intended to be installed in the laboratory of nuclear-physical methods of the element analysis of the Vinca Institute of Nuclear Sciences, Belgrade, Serbia. The cyclotron system ensures production of a beam of protons with energy in the range from 1 to 3 MeV with a spectrum width not more than 0.1%. The equipment of the cyclotron system has been manufactured and tested on test facilities in the D.V. Efremov Institute. Циклотронний комплекс СС1-3 призначений для оснащення лабораторії ядерно-фізичних методів елементного аналізу Інституту ядерних наук Вінча, Белград, Сербія. Циклотронний комплекс забезпечує отримання пучка протонів з енергією в діапазоні від 1 до 3 МеВ при ширині спектра не більше 0,1%. Обладнання циклотронного комплексу виготовлено та випробувано на стендах НІІЕФА ім. Д.В. Єфремова. Циклотронный комплекс СС1-3 предназначен для оснащения лаборатории ядерно-физических методов элементного анализа Института ядерных наук Винча, Белград, Сербия. Циклотронный комплекс обеспечивает получение пучка протонов с энергией в диапазоне от 1 до 3 МэВ при ширине спектра не более 0,1%. Оборудование циклотронного комплекса изготовлено и испытано на стендах НИИЭФА им. Д.В. Ефремова. 2013 Article The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis / O.L. Veresov, Yu.N. Gavrish, A.V. Galchuck, S.V. Grigorenko, V.I. Grigoriev, M.A. Emelianov, L.E. Korolev, A.N. Kuzhlev, I.I. Mezhov, V.G. Mudrolyubov, A.P. Strokach, S.S. Tsygankov, V.D. Shiltsev // Вопросы атомной науки и техники. — 2013. — № 6. — С. 13-15. — англ. 1562-6016 PACS: 29.20.dg https://nasplib.isofts.kiev.ua/handle/123456789/111809 en Вопросы атомной науки и техники application/pdf Національний науковий центр «Харківський фізико-технічний інститут» НАН України |
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| topic |
Состояние действующих и проекты новых ускорителей Состояние действующих и проекты новых ускорителей |
| spellingShingle |
Состояние действующих и проекты новых ускорителей Состояние действующих и проекты новых ускорителей Veresov, O.L. Gavrish, Yu.N. Galchuck, A.V. Grigorenko, S.V. Grigoriev, V.I. Emelianov, M.A. Korolev, L.E. Kuzhlev, A.N. Mezhov, I.I. Mudrolyubov, V.G. Strokach, A.P. Tsygankov, S.S. Shiltsev, V.D. The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis Вопросы атомной науки и техники |
| description |
The СС1-3 cyclotron system is intended to be installed in the laboratory of nuclear-physical methods of the element analysis of the Vinca Institute of Nuclear Sciences, Belgrade, Serbia. The cyclotron system ensures production of a beam of protons with energy in the range from 1 to 3 MeV with a spectrum width not more than 0.1%. The equipment of the cyclotron system has been manufactured and tested on test facilities in the D.V. Efremov Institute. |
| format |
Article |
| author |
Veresov, O.L. Gavrish, Yu.N. Galchuck, A.V. Grigorenko, S.V. Grigoriev, V.I. Emelianov, M.A. Korolev, L.E. Kuzhlev, A.N. Mezhov, I.I. Mudrolyubov, V.G. Strokach, A.P. Tsygankov, S.S. Shiltsev, V.D. |
| author_facet |
Veresov, O.L. Gavrish, Yu.N. Galchuck, A.V. Grigorenko, S.V. Grigoriev, V.I. Emelianov, M.A. Korolev, L.E. Kuzhlev, A.N. Mezhov, I.I. Mudrolyubov, V.G. Strokach, A.P. Tsygankov, S.S. Shiltsev, V.D. |
| author_sort |
Veresov, O.L. |
| title |
The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis |
| title_short |
The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis |
| title_full |
The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis |
| title_fullStr |
The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis |
| title_full_unstemmed |
The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis |
| title_sort |
сс1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis |
| publisher |
Національний науковий центр «Харківський фізико-технічний інститут» НАН України |
| publishDate |
2013 |
| topic_facet |
Состояние действующих и проекты новых ускорителей |
| url |
https://nasplib.isofts.kiev.ua/handle/123456789/111809 |
| citation_txt |
The СС1-3 cyclotron system for non-destructive nuclear-physical methods of the element analysis / O.L. Veresov, Yu.N. Gavrish, A.V. Galchuck, S.V. Grigorenko, V.I. Grigoriev, M.A. Emelianov, L.E. Korolev, A.N. Kuzhlev, I.I. Mezhov, V.G. Mudrolyubov, A.P. Strokach, S.S. Tsygankov, V.D. Shiltsev // Вопросы атомной науки и техники. — 2013. — № 6. — С. 13-15. — англ. |
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Вопросы атомной науки и техники |
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ISSN 1562-6016. ВАНТ. 2013. №6(88) 13
THE СС1-3 CYCLOTRON SYSTEM
FOR NON-DESTRUCTIVE NUCLEAR-PHYSICAL METHODS
OF THE ELEMENT ANALYSIS
O.L. Veresov, Yu.N. Gavrish, A.V. Galchuck, S.V. Grigorenko, V.I. Grigoriev,
M.A. Emelianov, L.E. Korolev, A.N. Kuzhlev, I.I. Mezhov, V.G. Mudrolyubov, A.P. Strokach,
S.S. Tsygankov, V.D. Shiltsev
FSUE “D.V. Efremov Scientific Research Institute of Electrophysical Apparatus”,
Saint-Petersburg, Russia
E-mail: npkluts@niiefa.spb.su
The СС1-3 cyclotron system is intended to be installed in the laboratory of nuclear-physical methods of the ele-
ment analysis of the Vinca Institute of Nuclear Sciences, Belgrade, Serbia. The cyclotron system ensures production
of a beam of protons with energy in the range from 1 to 3 MeV with a spectrum width not more than 0.1%. The
equipment of the cyclotron system has been manufactured and tested on test facilities in the D.V. Efremov Institute.
PACS: 29.20.dg
The СС1-3 cyclotron system has been designed at
the D.V. Efremov Scientific Research Institute of Elec-
trophysical Apparatus (NIIEFA), St.-Petersburg. The
system will ensure effective technological facilities nec-
essary to carry out analytical research in the Vinca Insti-
tute, Belgrade, Serbia in particular RBS, PES, NRA и
PIXE spectroscopies. Strict requirements are imposed
by the End User for parameters of accelerated proton
beams: the energy range should be from 1 to 3 MeV,
spectrum width no more than 0.1%, accuracy of energy
setting not worse than 1 keV and current ranging from
10 to 100 nA.
To attain the aforementioned parameters, we have
chosen the version of the system consisting of a com-
pact cyclotron with a beam-forming system (Fig. 1) and
systems of power supply, automatic control, vacuum
pumping and water cooling.
Fig. 1. The CC1-3 cyclotron with a beam-forming system
The compact cyclotron is intended to accelerate neg-
ative hydrogen ions. An extraction by stripping on a thin
carbon foil allows a proton beam with a final energy
variable in the range of 1…3 MeV to be delivered. The
current of the extracted beam of protons is 20 µA. The
cyclotron comprises the following units and elements:
an electromagnet with a vacuum chamber, resonance
system, probes and stripping device, external injection
system and high-frequency generator.
The major part of the cyclotron is a four-sector shield-
ing-type electromagnet (Fig. 2). The electromagnet is
1400 mm in dia, pole diameter is 600 mm and average
induction is 0.98 T. Gap hills/values are 50/100 mm. The
maximum acceleration radius for the 3 MeV energy is
250 mm. The power consumption of the magnet is
5.2 kW; its mass is 6.5 tons. The upper beam of the
magnet can be moved upward up to 500 mm.
Fig. 2. The magnet of the СС1-3 cyclotron
The vacuum chamber of the cyclotron (Fig. 3) con-
sists of a casing and two covers. The casing is a hollow
thick-walled cylinder of carbon steel, which simultane-
ously is a part of the iron core. Pole pieces of the mag-
net with welded rings of stainless steel are the covers of
the chamber. A cryogenic pump, vacuum chamber of the
matching magnet, RF power in-feeding device, AFT
trimmer, stripping device and probes are fastened to
flanges of the vacuum chamber casing.
The resonance accelerating system is located com-
pletely inside the vacuum chamber volume and is fixed
to a side surface of the vacuum chamber casing. The
system consists of two mirror-symmetrical quarter-wave
resonators (see Fig. 3). An inner conductor of each res-
onator consists of a dee and a stem. The dees in the vi-
cinity of the magnet axis are galvanically coupled. An
outer conductor of the system is claddings of the magnet
and vacuum chamber valleys as well as plates connect-
mailto:npkluts@niiefa.spb.su
ISSN 1562-6016. ВАНТ. 2013. №6(88) 14
ing the upper and lower claddings of chamber. The side
surfaces of the valley claddings follow the shape of the
side surfaces of the magnet sectors and serve as dummy
dees. The system is equipped with an inductive RF
power in-feeding device, AFT trimmer and RF-probe.
Stems, dees and claddings are cooled with water. The
central part of the dees is made removable and it is
cooled by thermal contact with the dees. The operating
frequency of the resonance system is 59.7 MHz and it
corresponds to the 4th harmonic of the revolution fre-
quency for hydrogen ions. The power of active losses in
each resonator is 1.6 kW at an RF voltage amplitude of
20 kV.
Fig. 3. The resonance system of the CC1-3 cyclotron
The high-frequency generator consists of a control
and stabilization module and RF-power amplifier. The
main parameters of the high-frequency generator are as
follows: operating frequency 59.7 MHz, frequency
stability 1.10-7, phase stability ±0.5°, output power
5 kW and accelerating voltage amplitude stability 10- 3.
Generator triode 3CW5000A7 is used in the power am-
plifier. The RF power is transmitted to the resonance
system through a flexible coaxial feeder.
In the process of designing we considered three ver-
sions of generation of a negative ion beam: radial or ax-
ial inner sources and an external injection system. Strin-
gent requirements are imposed on the energy spectrum
of the accelerated ion beam and current stability, there-
fore the last version of the aforementioned has been
chosen. The external injection system is located under
the electromagnet (Fig. 4).
Fig. 4. The external injection system
It consists of a source of negative ions with an ion-
optical system for the beam additional acceleration and
focusing, differential pumping chamber, two electrostat-
ic lenses, spiral inflector and ancillary equipment. The
ion beam current at the injector output is 0.5 mA, ion
energy is 11.5 keV, calculated normalized emittance is
not more than 0.3 π mm·mrad.
The cyclotron is equipped with two probes designed
for removal of the maximum beam power of 60 W. The
probes have similar connection dimensions and are
equipped with similar electrical and water connectors. A
remote drive ensures radial travel of the probes from the
minimum allowed position of ~ 100 mm to the position
when the probes are outside the acceleration area. The
stripping device is also equipped with a drive, which al-
lows one of three charge-exchange foils to be quickly
installed to the working position, and also the foil radius
and angle of location to be varied. The charge-exchange
foil is a carbon film of 0.2 µm thickness with a glue
substrate. We were not sure if this foil would suit us as
1 MeV ions lose ~15 keV when passing through the foil.
In this connection, pilot samples of this foil were manu-
factured and successfully tested on the operating cyclo-
tron СС-18/9 with anion energy of 1…2 MeV. Simulta-
neously, a technique for fabrication of foils with a
smaller thickness (not more than 1µ) has been devel-
oped and tried out, which will allow energy losses to be
reduced and reliability of the stripping device to be in-
creased.
The beam-forming system is designed to satisfy re-
quirements for the beam energy spectrum, which are not
typical for cyclotrons. The beam-forming system in-
cludes a matching magnet, a switching magnet, a dou-
blet of quadrupole lens, correcting magnets and an ana-
lyzing magnet (Fig. 5).
Fig. 5. The beam-forming system
The matching magnet is intended to make coincident
the axis of the extracted beam with the ion guide axis. A
doublet of quadrupole lenses focuses the beam to the
input slit of the analyzer. The switching magnet speci-
fies the beam bending angle for its further transport, ei-
ther 0° or ±15°. To measure parameters of the beam
transported to targets, the beam transport system con-
tains the following diagnostic means: beam profile mon-
itors (scanners), which are used to measure the beam
profile in horizontal and vertical planes, and Faraday
cups to measure the beam current.
The major part of the beam-forming system is an an-
alyzer, which consists of an analyzing magnet and col-
limators installed at the inlet and outlet of the analyzing
magnet vacuum chamber. The analyzing magnet (Fig. 6)
ISSN 1562-6016. ВАНТ. 2013. №6(88) 15
ensures a bending angle of 270° with a bending radius
of 600 mm. To expand the potentialities of the beam-
forming system, three fixed dimensions of the input and
output collimator slits of 0.5, 1 and 2 mm are provided.
The design energy resolution behind the output slit is
not worse than 0.05%.
The power supply system is intended to supply elec-
tric power to the cyclotron equipment. The maximum
(installed) power of the equipment is 40 kW. The system
consists of a power switchboard, two power supply
racks for magnets and lenses and two power supply
racks for the external injection system as well as power
supply units for step motors and the mechanism moving
upward the upper beam of the magnet.
The power switchboard distributes electric power to
primary consumers, and protects cable lines from long-
term overloads and cable faults.
Fig. 6. The analyzing magnet
The automatic control system is of distributed archi-
tecture. It consists of Mitsubishi and Fastwel IO control-
lers and computers, each being responsible for the con-
trol of one or several sub-systems of the cyclotron.
The main unit of the control system is an industrial
(host) computer, which inquires slave controllers and
transmits the information acquired to computers of the
operator’s workstation; receives commands from the
operator’s workstation and performs their arbitration
and distribution. Data exchange is realized via network
interfaces of three types: the Ethernet, an upper level
network, the ProfiBus DP and RS-485, low-level net-
works.
The Ethernet networks the host Mitsubishi control-
ler, which is responsible for the control, interlock and
signaling sub-system, the host computer, computers of
the operator’s workstation, computer of the beam cur-
rent measuring system and an industrial computer,
which controls the RF system. The ProfiBus DP links
the host controller, controllers of devices of the cyclo-
tron, and beam-forming system, vacuum system, power
switchboard, power supply racks of the external injec-
tion system, water cooling system as well as control
units of the power supply system of magnets and lenses.
The RS-485 networks the host computer, vacuum meas-
uring units and controllers of turbomolecular pumps as
well as the computer of the beam current measuring sys-
tem and drivers of step motors of devices for measuring
the beam current density. In addition, the RS-485 links
the controller of the cyclotron and beam-forming system
devices with drivers of step motors of probes and the
stripping device.
The vacuum system contains a cryogenic pump used
in the vacuum chamber of the cyclotron, four turbomo-
lecular pumps for the external injection system and
beam-forming system, mechanical dry pumps, gate
valves, valves, leak valves and pressure gages to meas-
ure low and high vacuum.
The equipment of the cyclotron will be cooled with
distilled water circulating in the water-cooling loop of
the cyclotron building. Four water distribution boards
are used to distribute cooling water to remove the heat
released by the heat-loaded components and units of the
cyclotron, to control pressure and stabilize water flow
rates.
By the present moment, the equipment has been de-
signed, manufactured, tested at test-facilities of the
D.V. Efremov Institute and made ready for delivery to
the Vinca Institute of Nuclear Science.
Article received 30.09.2013
ЦИКЛОТРОННЫЙ КОМПЛЕКС СС1-3 ДЛЯ НЕРАЗРУШАЮЩИХ ЯДЕРНО-ФИЗИЧЕСКИХ
МЕТОДОВ ЭЛЕМЕНТНОГО АНАЛИЗА
О.Л. Вересов, Ю.Н. Гавриш, А.В. Галчук, С.В. Григоренко, В.И. Григорьев, М.А. Емельянов, Л.Е. Королев,
А.Н. Кужлев, И.И. Межов, В.Г. Мудролюбов, А.П. Строкач, С.С. Цыганков, В.Д. Шильцев
Циклотронный комплекс СС1-3 предназначен для оснащения лаборатории ядерно-физических методов
элементного анализа Института ядерных наук Винча, Белград, Сербия. Циклотронный комплекс обеспечи-
вает получение пучка протонов с энергией в диапазоне от 1 до 3 МэВ при ширине спектра не более 0,1%.
Оборудование циклотронного комплекса изготовлено и испытано на стендах НИИЭФА им. Д.В. Ефремова.
ЦИКЛОТРОННИЙ КОМПЛЕКС СС1-3 ДЛЯ НЕРУЙНІВНИХ ЯДЕРНО-ФІЗИЧНИХ МЕТОДІВ
ЕЛЕМЕНТНОГО АНАЛІЗУ
О.Л. Вересов, Ю.М. Гавриш, А.В. Галчук, С.В. Григоренко, В.І. Григорьєв, М.А. Ємельянов, Л.Є. Корольов,
А.Н. Кужлев, І.І. Межов, В.Г. Мудролюбов, А.П. Строкач, С.С. Циганков, В.Д. Шильцев
Циклотронний комплекс СС1-3 призначений для оснащення лабораторії ядерно-фізичних методів елеме-
нтного аналізу Інституту ядерних наук Вінча, Белград, Сербія. Циклотронний комплекс забезпечує отри-
мання пучка протонів з енергією в діапазоні від 1 до 3 МеВ при ширині спектра не більше 0,1%. Обладнання
циклотронного комплексу виготовлено та випробувано на стендах НІІЕФА ім. Д.В. Єфремова.
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