Cross sections for production of 43Sc, 44Sc, and 46Sc isotopes in the 45Sc + 3He reaction

Reactions 45 Sc( 3 He, α n ) 43 Sc, 45 Sc( 3 He, α) 44 Sc, and 45 Sc( 3 He, 2 p ) 46 Sc, resulting from the irradiation of scandium targets with a beam of 3 He ions with energy from 5 to 24 MeV, are investigated in experiments on the U120M cyclotron of the Nuclear Physics Institute (Rez, Czech Repub...

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Veröffentlicht in:Physics of particles and nuclei letters 2013-09, Vol.10 (5), p.410-414
Hauptverfasser: Skobelev, N. K., Kulko, A. A., Penionzhkevich, Yu. E., Voskoboinik, E. I., Kroha, V., Burjan, V., Hons, Z., Mrázek, J., Piskoř, Š., Šimečkova, E.
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container_end_page 414
container_issue 5
container_start_page 410
container_title Physics of particles and nuclei letters
container_volume 10
creator Skobelev, N. K.
Kulko, A. A.
Penionzhkevich, Yu. E.
Voskoboinik, E. I.
Kroha, V.
Burjan, V.
Hons, Z.
Mrázek, J.
Piskoř, Š.
Šimečkova, E.
description Reactions 45 Sc( 3 He, α n ) 43 Sc, 45 Sc( 3 He, α) 44 Sc, and 45 Sc( 3 He, 2 p ) 46 Sc, resulting from the irradiation of scandium targets with a beam of 3 He ions with energy from 5 to 24 MeV, are investigated in experiments on the U120M cyclotron of the Nuclear Physics Institute (Rez, Czech Republic). The activation technique is used to find the yield of the produced Sc isotopes. The induced γ activity in the targets is measured using a high-resolution HPGe detector. Despite the low binding energy of 3 He and positive reaction Q values, which leads to formation of the 44 Sc and 46 Sc isotopes, the behavior of the excitation functions for the formation of these isotopes differs from the behavior of the excitation function for deuterons. Scandium-44 formation cross sections reach their maximum at the reaction Coulomb barrier. This is because not only 44 Sc but also a stable 4 He nucleus is formed in the reaction.
doi_str_mv 10.1134/S1547477113050142
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Despite the low binding energy of 3 He and positive reaction Q values, which leads to formation of the 44 Sc and 46 Sc isotopes, the behavior of the excitation functions for the formation of these isotopes differs from the behavior of the excitation function for deuterons. Scandium-44 formation cross sections reach their maximum at the reaction Coulomb barrier. This is because not only 44 Sc but also a stable 4 He nucleus is formed in the reaction.</description><identifier>ISSN: 1547-4771</identifier><identifier>EISSN: 1531-8567</identifier><identifier>DOI: 10.1134/S1547477113050142</identifier><language>eng</language><publisher>Boston: Springer US</publisher><subject>Particle and Nuclear Physics ; Physics ; Physics and Astronomy ; Physics of Elementary Particles and Atomic Nuclei. 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Nuclei Lett</stitle><date>2013-09</date><risdate>2013</risdate><volume>10</volume><issue>5</issue><spage>410</spage><epage>414</epage><pages>410-414</pages><issn>1547-4771</issn><eissn>1531-8567</eissn><abstract>Reactions 45 Sc( 3 He, α n ) 43 Sc, 45 Sc( 3 He, α) 44 Sc, and 45 Sc( 3 He, 2 p ) 46 Sc, resulting from the irradiation of scandium targets with a beam of 3 He ions with energy from 5 to 24 MeV, are investigated in experiments on the U120M cyclotron of the Nuclear Physics Institute (Rez, Czech Republic). The activation technique is used to find the yield of the produced Sc isotopes. The induced γ activity in the targets is measured using a high-resolution HPGe detector. Despite the low binding energy of 3 He and positive reaction Q values, which leads to formation of the 44 Sc and 46 Sc isotopes, the behavior of the excitation functions for the formation of these isotopes differs from the behavior of the excitation function for deuterons. 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Physics and Astronomy
Physics of Elementary Particles and Atomic Nuclei. Experiment
title Cross sections for production of 43Sc, 44Sc, and 46Sc isotopes in the 45Sc + 3He reaction
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