Ratio of Gamow-Teller to Fermi Strength Observed in 13,14C(p,n) at 492 and 590 Mev View Full Text


Ontology type: schema:Chapter     


Chapter Info

DATE

1988

AUTHORS

J. L. Ullmann , J. Rapaport , P. W. Lisowski , R. C. Byrd , T. Carey , T. N. Taddeucci , J. McClelland , L. Rybarcyk , R. C. Haight , N. S. P. King , G. L. Morgan , D. A. Lind , R. Smythe , C. D. Zafiratos , D. Prout , E. Sugarbaker , W. P. Alford , W. G. Love

ABSTRACT

It has been recognized for a number of years that certain spin-isospin components of the nucleon-nucleus effective interaction can be inferred from (p,n) reactions to states of known nuclear structure. For L = 0, S = 0 and L = 0, S = 1 transitions, the 0-degree (p,n) cross section can be related respectively to Fermi and Gamow-Teller beta decay matrix elements1. If these transitions occur in the same nucleus, the ratio of isovector spin-flip to non-spin-flip effective interactions can be measured without regard for absolute normalization. The best reaction to measure this is 14C(p,n) which goes by a pure Gamow-Teller transition to the 1+ state at 3.95 MeV in 14N, and Fermi transition to the 2.31 MeV 0+ state. This work extends the ratio measurements made at lower energies (ref. 1, 2, 3) to 492 and 590 MeV. More... »

PAGES

245-250

Identifiers

URI

http://scigraph.springernature.com/pub.10.1007/978-1-4613-0769-3_21

DOI

http://dx.doi.org/10.1007/978-1-4613-0769-3_21

DIMENSIONS

https://app.dimensions.ai/details/publication/pub.1016278436


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