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7Be yield produced in secondary reactions in a nuclear reactor

7Be yield produced in secondary reactions in a nuclear reactor Atomic Energy, Vol. 104, No. 1, 2008 Be YIELD PRODUCED IN SECONDARY REACTIONS IN A NUCLEAR REACTOR S. Mukhammedov, A. Khaidarov, UDC 621.039.574.5 and E. G. Barsukova The yield of a radionuclide is an important physical quantity, determining the number of radioactive atoms in the irradiated samples. For low and intermediate energy protons and deuterons, Be forms from lithium and boron in the nucle- 7 10 11 6 7 10 11 ar reactions Li (p, n), B (p, α), B (p, αn), Li (d, n), Li (d,2n), B (d, αn), B (d, α2n). For purposes of using a cyclotron in activation analysis, the Be yield obtained by irradiating targets with charged particles accelerated in the U-150 cyclotron at the Institute of Nuclear Physics of the Academy of Sciences of the Republic of Uzbekistan was investigated [1–5]. The yield of Be in the reactions Li(d, n) and Be(d, n) was also measured at deuteron energies 25 and 40 MeV [5]. Another method for obtaining Be consists in using recoil protons and deuterons which form in a nuclear reactor as a result of (n, p) or (n, d) and elastic or inelastic scattering of fast neutrons interacting with hydrogen nuclei [6]. http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.png Atomic Energy Springer Journals

7Be yield produced in secondary reactions in a nuclear reactor

Mukhammedov, S.; Khaidarov, A.; Barsukova, E.
Atomic Energy , Volume 104 (1) – Apr 19, 2008
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References (6)

Publisher
Springer Journals
Copyright
Copyright © 2008 by Springer Science+Business Media, Inc.
Subject
Engineering; Nuclear Engineering; Nuclear Physics, Heavy Ions, Hadrons; Nuclear Chemistry
ISSN
1063-4258
eISSN
1573-8205
DOI
10.1007/s10512-008-0012-z
Publisher site
See Article on Publisher Site

Abstract

Atomic Energy, Vol. 104, No. 1, 2008 Be YIELD PRODUCED IN SECONDARY REACTIONS IN A NUCLEAR REACTOR S. Mukhammedov, A. Khaidarov, UDC 621.039.574.5 and E. G. Barsukova The yield of a radionuclide is an important physical quantity, determining the number of radioactive atoms in the irradiated samples. For low and intermediate energy protons and deuterons, Be forms from lithium and boron in the nucle- 7 10 11 6 7 10 11 ar reactions Li (p, n), B (p, α), B (p, αn), Li (d, n), Li (d,2n), B (d, αn), B (d, α2n). For purposes of using a cyclotron in activation analysis, the Be yield obtained by irradiating targets with charged particles accelerated in the U-150 cyclotron at the Institute of Nuclear Physics of the Academy of Sciences of the Republic of Uzbekistan was investigated [1–5]. The yield of Be in the reactions Li(d, n) and Be(d, n) was also measured at deuteron energies 25 and 40 MeV [5]. Another method for obtaining Be consists in using recoil protons and deuterons which form in a nuclear reactor as a result of (n, p) or (n, d) and elastic or inelastic scattering of fast neutrons interacting with hydrogen nuclei [6].

Journal

Atomic Energy – Springer Journals

Published: Apr 19, 2008

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