The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam

Cross sections of fission reactions of ¹⁹⁷Au, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U heavy metals induced by protons with energy of 0.66 GeV are presented. The protons beam was extracted from the Phasotron accelerator at JINR, Dubna, Russian Federation. Fission reactions cross sections were measured using solid...

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Datum:2017
Hauptverfasser: Zhuk, I., Husak, K., Kruk, A., Voronko, V., Sotnikov, V., Zadan, А., Baldin, А., Tyutyunnikov, S.
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Veröffentlicht: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2017
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Zitieren:The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam / I. Zhuk, K. Husak, A. Kruk, V. Voronko, V. Sotnikov, А. Zadan, А. Baldin, S. Tyutyunnikov // Вопросы атомной науки и техники. — 2017. — № 6. — С. 145-147. — Бібліогр.: 13 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
id nasplib_isofts_kiev_ua-123456789-136190
record_format dspace
spelling Zhuk, I.
Husak, K.
Kruk, A.
Voronko, V.
Sotnikov, V.
Zadan, А.
Baldin, А.
Tyutyunnikov, S.
2018-06-16T06:55:01Z
2018-06-16T06:55:01Z
2017
The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam / I. Zhuk, K. Husak, A. Kruk, V. Voronko, V. Sotnikov, А. Zadan, А. Baldin, S. Tyutyunnikov // Вопросы атомной науки и техники. — 2017. — № 6. — С. 145-147. — Бібліогр.: 13 назв. — англ.
1562-6016
PACS: 24.90+d, 28.65+a, 29.40Wk
https://nasplib.isofts.kiev.ua/handle/123456789/136190
Cross sections of fission reactions of ¹⁹⁷Au, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U heavy metals induced by protons with energy of 0.66 GeV are presented. The protons beam was extracted from the Phasotron accelerator at JINR, Dubna, Russian Federation. Fission reactions cross sections were measured using solid state nuclear track detectors (SSNTD) and activation gamma-spectroscopy. The comparison with results from others researchers were done. The obtained results would be added in the international databases for testing of programme code for ADS-systems.
Представлені експериментальні дані по перетинах реакцій поділу ядер важких металів ¹⁹⁷Au, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U під дією протонів з енергією 0,66 ГеВ. Експерименти проведені на пучках протонів прискорювача Фазатрон, ОІЯД, Дубна, РФ. Для визначення перетинів реакцій поділу використана комплексна методика твердотільних трекових детекторів ядер і активаціонної гамма-спектрометрії. Виконано порівняння отриманих результатів з результатами інших дослідників. Отримані результати доповнять базу експериментальних ядерних даних, що дозволить протестувати комп'ютерні коди, що застосовуються при розрахунках параметрів ADS.
Представлены экспериментальные данные по сечениям реакций деления ядер тяжелых металлов ¹⁹⁷Au, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U под действием протонов с энергией 0,66 ГэВ. Эксперименты проведены на пучках протонов ускорителя Фазатрон, ОИЯИ, Дубна, РФ. Для определения сечений реакций деления использована комплексная методика твердотельных трековых детекторов ядер и активационной гамма-спектрометрии. Выполнено сравнение полученных результатов с результатами других исследователей. Полученные результаты дополнят базу экспериментальных ядерных данных, что позволит протестировать компьютерные коды, применяемые при расчетах параметров ADS.
en
Національний науковий центр «Харківський фізико-технічний інститут» НАН України
Вопросы атомной науки и техники
Применение ядерных методов
The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam
Експериментальне вивчення перетинів реакцій поділу ядер важких металів протонами з енергією 0,66 ГеВ
Экспериментальное изучение сечений реакций деления ядер тяжелых металлов протонами с энергией 0,66 ГэВ
Article
published earlier
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
title The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam
spellingShingle The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam
Zhuk, I.
Husak, K.
Kruk, A.
Voronko, V.
Sotnikov, V.
Zadan, А.
Baldin, А.
Tyutyunnikov, S.
Применение ядерных методов
title_short The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam
title_full The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam
title_fullStr The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam
title_full_unstemmed The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam
title_sort experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 gev protons beam
author Zhuk, I.
Husak, K.
Kruk, A.
Voronko, V.
Sotnikov, V.
Zadan, А.
Baldin, А.
Tyutyunnikov, S.
author_facet Zhuk, I.
Husak, K.
Kruk, A.
Voronko, V.
Sotnikov, V.
Zadan, А.
Baldin, А.
Tyutyunnikov, S.
topic Применение ядерных методов
topic_facet Применение ядерных методов
publishDate 2017
language English
container_title Вопросы атомной науки и техники
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
format Article
title_alt Експериментальне вивчення перетинів реакцій поділу ядер важких металів протонами з енергією 0,66 ГеВ
Экспериментальное изучение сечений реакций деления ядер тяжелых металлов протонами с энергией 0,66 ГэВ
description Cross sections of fission reactions of ¹⁹⁷Au, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U heavy metals induced by protons with energy of 0.66 GeV are presented. The protons beam was extracted from the Phasotron accelerator at JINR, Dubna, Russian Federation. Fission reactions cross sections were measured using solid state nuclear track detectors (SSNTD) and activation gamma-spectroscopy. The comparison with results from others researchers were done. The obtained results would be added in the international databases for testing of programme code for ADS-systems. Представлені експериментальні дані по перетинах реакцій поділу ядер важких металів ¹⁹⁷Au, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U під дією протонів з енергією 0,66 ГеВ. Експерименти проведені на пучках протонів прискорювача Фазатрон, ОІЯД, Дубна, РФ. Для визначення перетинів реакцій поділу використана комплексна методика твердотільних трекових детекторів ядер і активаціонної гамма-спектрометрії. Виконано порівняння отриманих результатів з результатами інших дослідників. Отримані результати доповнять базу експериментальних ядерних даних, що дозволить протестувати комп'ютерні коди, що застосовуються при розрахунках параметрів ADS. Представлены экспериментальные данные по сечениям реакций деления ядер тяжелых металлов ¹⁹⁷Au, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U под действием протонов с энергией 0,66 ГэВ. Эксперименты проведены на пучках протонов ускорителя Фазатрон, ОИЯИ, Дубна, РФ. Для определения сечений реакций деления использована комплексная методика твердотельных трековых детекторов ядер и активационной гамма-спектрометрии. Выполнено сравнение полученных результатов с результатами других исследователей. Полученные результаты дополнят базу экспериментальных ядерных данных, что позволит протестировать компьютерные коды, применяемые при расчетах параметров ADS.
issn 1562-6016
url https://nasplib.isofts.kiev.ua/handle/123456789/136190
citation_txt The experimental determination of heavy metal nuclei fission reactions cross sections at 0.66 GeV protons beam / I. Zhuk, K. Husak, A. Kruk, V. Voronko, V. Sotnikov, А. Zadan, А. Baldin, S. Tyutyunnikov // Вопросы атомной науки и техники. — 2017. — № 6. — С. 145-147. — Бібліогр.: 13 назв. — англ.
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fulltext ISSN 1562-6016. ВАНТ. 2017. №6(112) 145 THE EXPERIMENTAL DETERMINATION OF HEAVY METAL NUCLEI FISSION REACTIONS CROSS SECTIONS AT 0.66 GeV PROTONS BEAM I. Zhuk 1 , K. Husak 1 , A. Kruk 1 , V. Voronko 2 , V. Sotnikov 2 , А. Zadan 2 , А. Baldin 3 , S. Tyutyunnikov 3 1 State Scientific Institution “The Joint Institute for Power and Nuclear Research – Sosny” of National Academy of Sciences, Minsk, Republic of Belarus; 2 National Science Center “Kharkov Institute of Physics and Technology”, Kharkov, Ukraine; 3 Joint Institute for Nuclear Research, Dubna, Russian Federation E-mail: lab13sosny@gmail.com Cross sections of fission reactions of 197 Au, 207 Pb, 209 Bi, 232 Th, 238 U heavy metals induced by protons with energy of 0.66 GeV are presented. The protons beam was extracted from the Phasotron accelerator at JINR, Dubna, Russian Federation. Fission reactions cross sections were measured using solid state nuclear track detectors (SSNTD) and activation gamma-spectroscopy. The comparison with results from others researchers were done. The obtained re- sults would be added in the international databases for testing of programme code for ADS-systems. PACS: 24.90+d, 28.65+a, 29.40Wk INTRODUCTION Since 2010 project “Energy and Transmutation of radioactive waste” carried out in Joint Institute for Nu- clear Research (Dubna, RF). In the frame of the project investigations are conducting on studies of different subcritical assemblies physics characteristics driven by protons and deuterons beams with 0.6…12.0 GeV ener- gies; multiplicities and spatial distributions of energy- time of neutron spectrum; possibility to energy produc- tion and utilization of radioactive waste studies on mas- sive natural uranium (depleted uranium) and thorium targets based on the relativistic nuclear technologies (RNT); studies of superconductors irradiation stability in neutrons and protons beams [1]. Option of target material is significant phase for ex- periment calculating and optimization of central target part irradiated by relativistic ions. Commonly neutron generating target are composed of Ta, Au, Bi, Hg, W, Pb, Th, U for accelerator driven system (ADS) [2]. Because of fission reaction is one of primary decay channel it is experimental data of fission reactions cross sections for energies up several GeV per nucleon are needed for creating of full-scale ADS. 1. EXPERIMENTAL TECHNIQUE AND EXPERIMENT DESCRIPTION 1.1. EXPERIMENTAL TECHNIQUE The solid state nuclear track detectors (SSNTD) method was chosen as a main method for fission reac- tions cross sections determination for this experiment. SSNTD technique is based on correlation between the track density on a track detector and a flux density of the investigated beam. Sensors made of track detectors placed in contact with a fission foil are irradiated by the beam. Fission fragments produced in fission reactions in fission foils form tracks on the track detectors surface. Sensor SSNTD is sketched on Fig. 1. There white section is artificial mica. The used method is described at greater length in [3]. Fig. 1. Irradiated setup scheme and photo In accordance with [3] nuclide cross section i is defined: i sensi q q PN k   . (1) There i qN  track density on a track detector which placed in contact with a fission foil, sens qk – calibration factor for «fission foil + SSNTD»; и P – primary parti- cles number. In general calibration factor determine in the follow- ing way: isens i q q q q Ak d  , (2) где iA  number of charged particles produced in the fission reaction of i-nuclides; i  the fraction of charged particles reaching the detector in the fission reaction of i-nuclides; q  detection efficiency of the charged particle track detectors; qd  i-layer thickness of nuclides in the radiator, cm; q  nuclear density of i-nuclides in the radiator, nuclei/сm 3 . Calibration factors is used from [4] for this experi- ment. For fission reaction i determines, in accordance with [3] as: 0 0 0 0 0 1 1 for 2 2 1 for 4 1 for , 4 q q i q q q d d R R d R R d R d                      (3) where 0R  average fission fragments range. ISSN 1562-6016. ВАНТ. 2017. №6(112) 146 In this work thick radiators were used. In the context of SSNTD technique “thick” radiator means that the radiator thickness is exceeded significantly the mean free path of fission fragments in the radiator material ( Rd 0q  ). This circumstance allows to reject an uncertainty caused by radiator thickness determination (as for thin foils) and to increase the total number of fission frag- ments. At the same time, due to the radiator thickness, we can register the only one fission fragment from the binary fission process and cannot distinguish it by using two correlated tracks. So, the fission process cannot be discriminated from the other high energy processes (such as spallation, multifragmentation and strong asymmetric fission) in which heavy and medium mass particles can be generated [5]. FLUKA [6], intranuclear cascade model and the model of the nucleon-nucleon interactions RQMD-2.4 were applied to study this effect [7]. Correction for this effect is 6…10% depending on type and energy of incident particle. In addition, the influence of the kinematics of fission process on the track density on the track detectors has to be taking into account for the whole protons energy range. Pulse transfer effect for fission fragments can be compensated by the “sandwich-like” composition of sensors, which allows registering tracks in 4π geometry (BACK/FACE). Correction for this effect was calculat- ing in FLUKA and it is 0.5…2%. 1.2. EXPERIMENT DETAILS Irradiation of the setup was carried out with 0.66 GeV protons beam on the Phasotron accelerator at JINR, Dubna, Russian Federation. In this experiment artificial mica is used. It is condi- tioned by low effect of recoil nuclei. The used materials characteristics are present in Ta- ble 1. Table 1 The used materials characteristics The used materials Thickness, mm Diameter, mm Al 1.0 6.5 197 Au 0.030 6.5 207 Pb 0.500 6.5 209 Bi 0.025 6.5 232 Th 0.070 6.5 238 U 0.030 6.5 Artificial mica 0.030 6.5 The studied foils was placed into plexiglass shaped location plate (height = 1 сm and diameter = 6.5 mm). Before irradiation plexiglass shaped location plate fill by foil and mica (Fig. 1). Aluminium cylindrical sam- ples (height = 1 сm and diameter = 6.5 mm) put on up- per and lowest part of plexiglass shaped location plate. These samples are applied as activation detectors for determination protons flux. Setup was disassembled after irradiation. The SSNTD are etched in 6.8% HF solution with t = 60°C to make tracks "visible" in an optical microscope. Time etching is 10…45 min which depends on track density. To obtain an accurate measure of the track densities the tedious method of manual track counting is chosen. We count tracks in many photomicrographs produced for each detector using an optical microscope. 2. RESULTS AND DISCUSSION In Table 2 experimental data are presented. These are used for determining of heavy metal nuclei fission reactions cross sections induced by 0.66 GeV protons beam. Table 2 Experimental data and determinate values Nuclide Ratio “BACK/FACE” Average track density, track/сm 2 Fission cross- section, mb 197 Au 1.60±0.07 8.23·10 5 70±20 207 Pb 1.44±0.07 1.55·10 6 120±30 209 Bi 1.43±0.07 2.44·10 6 210±60 232 Th 1.22±0.05 8.57·10 6 750±200 238 U 1.24±0.05 1.06·10 7 950±260 Measured dependence of the ratio “BACK/FACE” decrease with atomic number increase is self-contained quantitativeness for verification of different theoretic models in describing of nuclei fission reactions by rela- tivistic particles (independent of uncertainties of inci- dent beam intensity measurement, corrections on detec- tor efficiency etc.). Probing uncertainties of beam monitoring adds main inaccuracy to measured result – about 10…15%. Finally it is ~ 50% from total relative measurement uncertainty. Extended measurement uncertainty was estimated by the international standard ISO/IEC 17025:1999 and it formed 30%. Similar data for deuterons are missed exclude sever- al studies [8]. In the frame of project “Energy and Transmutation of radioactive waste” were determined 181 Ta, 197 Au, 207 Pb, 209 Bi, 232 Th, 238 U heavy metals nuclei fission reactions cross-sections induced by deuterons with 2, 2.94 3.5 GeV per nucleon energies [9]. In whole, obtained data on fission reactions cross sections of 197 Au, 207 Pb, 209 Bi, 232 Th, 238 U by 0.66 GeV protons are in good agreement with experimental data in [8, 10 - 13], and with theoretical calculation from [8] (Figs. 2, 3). Fig. 2. Fission cross sections values of 232 Th, 238 U by protons ISSN 1562-6016. ВАНТ. 2017. №6(112) 147 Fig. 3. Fission cross sections values of 197 Au, 207 Pb, 209 Bi by protons Analysis of described experiment results and com- parison with other studies confirm that the SSNTD method make it possible to obtain correct and responsi- ble data on fission reactions cross sections for different type and energy of incident particles. REFERENCES 1. A.A. Baldin et al. Relativistic nuclear technology (RNT) for energy production and utilization of spent nuclear fuel. The results of first experiments on physical justification of RNT // Particles and Nuclei, Letters. 2011, v. 8, № 6(169), p. 1007-1023. 2. А.I. Obukhov. Nuclei fission in interaction with in- termediate-energies protons and neutrons // Physics of Particles and Nuclei. 2001, v. 32, Iss. 2, p. 319- 376. 3. А.P. Malikhin et al. Determination of fission density distribution by solid state nuclear track detectors in critical assemblies // Proc. Of NASB. Ser. Of phys.- en. sciences. 1970, № 2, p. 16-23. 4. S.R. Hashemi-Nezhad et al. 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Article received 25.09.2017 ЭКСПЕРИМЕНТАЛЬНОЕ ИЗУЧЕНИЕ СЕЧЕНИЙ РЕАКЦИЙ ДЕЛЕНИЯ ЯДЕР ТЯЖЕЛЫХ МЕТАЛЛОВ ПРОТОНАМИ С ЭНЕРГИЕЙ 0,66 ГэВ И. Жук, К. Гусак, А. Крюк, В. Воронко, В. Сотников, А. Жадан, А. Балдин, С. Тютюнников Представлены экспериментальные данные по сечениям реакций деления ядер тяжелых металлов 197 Au, 207 Pb, 209 Bi, 232 Th, 238 U под действием протонов с энергией 0,66 ГэВ. Эксперименты проведены на пучках протонов ускорителя Фазатрон, ОИЯИ, Дубна, РФ. Для определения сечений реакций деления использована комплексная методика твердотельных трековых детекторов ядер и активационной гамма-спектрометрии. Выполнено сравнение полученных результатов с результатами других исследователей. Полученные резуль- таты дополнят базу экспериментальных ядерных данных, что позволит протестировать компьютерные коды, применяемые при расчетах параметров ADS. ЕКСПЕРИМЕНТАЛЬНЕ ВИВЧЕННЯ ПЕРЕТИНІВ РЕАКЦІЙ ПОДІЛУ ЯДЕР ВАЖКИХ МЕТАЛІВ ПРОТОНАМИ З ЕНЕРГІЄЮ 0,66 ГеВ І. Жук, К. Гусак, А. Крюк, В. Воронко, В. Сотников, А. Жадан, А. Балдін, С. Тютюнників Представлені експериментальні дані по перетинах реакцій поділу ядер важких металів 197 Au, 207 Pb, 209 Bi, 232 Th, 238 U під дією протонів з енергією 0,66 ГеВ. Експерименти проведені на пучках протонів прискорювача Фазатрон, ОІЯД, Дубна, РФ. Для визначення перетинів реакцій поділу використана комплексна методика твердотільних трекових детекторів ядер і активаціонної гамма-спектрометрії. Виконано порівняння отрима- них результатів з результатами інших дослідників. Отримані результати доповнять базу експериментальних ядерних даних, що дозволить протестувати комп'ютерні коди, що застосовуються при розрахунках парамет- рів ADS.