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Isovector excitations in nuclei with composite projectiles: (3He, t), (d, 2He), and heavy ions

Publication: Canadian Journal of Physics
June 1987

Abstract

A variety of charge-exchange reactions involving complex particles has been used to study the response of a nucleus to a spin–isospin probe. The reactions have been the (3He, t) reaction, the (d, 2He) reaction, and reactions with the heavy ions 12C, 14N, 16O, and 20Ne as beam and charge exchange both ways. With all reactions, transitions are observed to the low-lying giant-resonance region, the quasi-elastic region, and the Δ region. With the (d, 2He) reaction, the spin structure of the response is studied.

Résumé

Diverses réactions d'échange de charge impliquant des particules complexes ont été utilisées pour étudier la réponse d'un noyau à une sonde spin–isospin. Ces réactions ont été la réaction (3He, t), la réaction (d, 2He) et des réactions avec les ions lourds 12C, 14N, 16O and 20Ne comme faisceau et échange de charge dans les deux sens. Pour toutes les réactions, on observe des transitions vers la région de résonance géante à basse énergie, la région quasi-élastique et la région Δ. Avec la réaction (d, 2He) la structure de spin de la réponse est étudiée.

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cover image Canadian Journal of Physics
Canadian Journal of Physics
Volume 65Number 6June 1987
Pages: 600 - 608

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Version of record online: 12 February 2011

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Cited by

1. Energy levels of light nuclei A= 12
2. Mechanisms of charge-exchange in the 12C(7Li, 7Be)12B reaction at the beam energy of 82 MeV
3. Δ mass in quasifree Δ production from C12
4. Δ excitation and coherent pion production in charge exchange reactions
5. Nucleon Charge-Exchange Reactions at Intermediate Energy
6. Energy levels of light nuclei, A = 20
7. Energy levels of light nuclei A = 16–17
8. The 12C(n, p)12B reaction at En = 98 MeV
9. Nuclear data sheets for A = 90
10. Nuclear spin and isospin excitations
11. Δ excitations in nuclei
12. Medium effects on Δ properties and N-Δ transition form factors
13. Energy levels of light nuclei A = 11−12

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