TY - JOUR
T1 - Gamow-Teller transition strengths in the intermediate nucleus of the 116Cd double-β decay by the 116Cd(p,n)116In and 116Sn(n,p)116In reactions at 300 MeV
AU - Sasano, M.
AU - Sakai, H.
AU - Yako, K.
AU - Wakasa, T.
AU - Dozono, M.
AU - Rodin, V.
AU - Faessler, A.
AU - Fujita, K.
AU - Greenfield, M. B.
AU - Hatanaka, K.
AU - Itoh, K.
AU - Kawabata, T.
AU - Kuboki, H.
AU - Maeda, Y.
AU - Miki, K.
AU - Muto, K.
AU - Noji, S.
AU - Okamura, H.
AU - Sakemi, Y.
AU - Sekiguchi, K.
AU - Shimizu, Y.
AU - Sasamoto, Y.
AU - Tameshige, Y.
AU - Tamii, A.
AU - Uesaka, T.
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 2012/6/6
Y1 - 2012/6/6
N2 - The double-differential cross sections for the 116Cd(p,n) and 116Sn(n,p) reactions were measured at 300 MeV for studying the nuclear matrix element of the 116Cd ββ decay. A multipole decomposition technique was applied to the spectra to extract the Gamow-Teller (GT) component. The integrated GT strengths up to an excitation energy of 30 MeV in the intermediate nucleus 116In are 40±6 and 11±1 in the (p,n) and (n,p) spectra, respectively, including the component from the isovector spin monopole (IVSM). The spectra are compared with those obtained from a theoretical calculation with a quasiparticle random phase approximation, where the contribution from the IVSM component as well as the interference effect between the GT and IVSM components are fully taken into account.
AB - The double-differential cross sections for the 116Cd(p,n) and 116Sn(n,p) reactions were measured at 300 MeV for studying the nuclear matrix element of the 116Cd ββ decay. A multipole decomposition technique was applied to the spectra to extract the Gamow-Teller (GT) component. The integrated GT strengths up to an excitation energy of 30 MeV in the intermediate nucleus 116In are 40±6 and 11±1 in the (p,n) and (n,p) spectra, respectively, including the component from the isovector spin monopole (IVSM). The spectra are compared with those obtained from a theoretical calculation with a quasiparticle random phase approximation, where the contribution from the IVSM component as well as the interference effect between the GT and IVSM components are fully taken into account.
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U2 - 10.1103/PhysRevC.85.061301
DO - 10.1103/PhysRevC.85.061301
M3 - Article
AN - SCOPUS:84862897864
SN - 0556-2813
VL - 85
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 6
M1 - 061301
ER -