TY - JOUR
T1 - Effects of spherical and deformed state mixing on the E2 rates between the odd-parity states of 40Ca
AU - Goode, Philip
N1 - Funding Information:
t Present Address: Department of Physics and Astronomy, University of Rochester, Rochester, N. Y. *t Work supported in part by the National Science Foundation.
Copyright:
Copyright 2014 Elsevier B.V., All rights reserved.
PY - 1970/1/19
Y1 - 1970/1/19
N2 - Several E2 decay schemes for the low-lying T = 0 odd-parity states of 40Ca are discussed. It is shown that a pure RPA description of these decays is not satisfactory. Gerace and Green have mixed these pure RPA states with 3p-3h deformed states to describe the T = 0 odd-parity states. In the calculation of the E2 rates with their wave functions, the intrinsic quadrupole moment of the band is taken to be a parameter so that several cases may be considered. It is thus shown that only once choice for the intrinsic quadrupole moment leads to a consistent explanation of the B(E2) values. Furthermore, the choice for the intrinsic quadrupole moment is the only one which is consistent with those of the even parity states in 40Ca.
AB - Several E2 decay schemes for the low-lying T = 0 odd-parity states of 40Ca are discussed. It is shown that a pure RPA description of these decays is not satisfactory. Gerace and Green have mixed these pure RPA states with 3p-3h deformed states to describe the T = 0 odd-parity states. In the calculation of the E2 rates with their wave functions, the intrinsic quadrupole moment of the band is taken to be a parameter so that several cases may be considered. It is thus shown that only once choice for the intrinsic quadrupole moment leads to a consistent explanation of the B(E2) values. Furthermore, the choice for the intrinsic quadrupole moment is the only one which is consistent with those of the even parity states in 40Ca.
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U2 - 10.1016/0375-9474(70)90575-0
DO - 10.1016/0375-9474(70)90575-0
M3 - Article
AN - SCOPUS:49849110224
SN - 0375-9474
VL - 140
SP - 481
EP - 493
JO - Nuclear Physics, Section A
JF - Nuclear Physics, Section A
IS - 3
ER -