The g factor of the 12 +K-isomer in 174W has been measured by means of the time-differential perturbed angular distribution technique as g(12 +) = + 0.304 (11). In addition, the half-life of the isomer has been remeasured as T1 / 2(12 +) = 124 (8) ns, in agreement with the literature value and confirming the anomalous hindrance F of the E2 transition to the 10 + level of the ground state band with respect to the γ-tunnelling model prediction. The measured g factor has been compared with estimates based on experimental g factors from odd-mass isotopes in the same mass region and with Nilsson model calculations. The results establish unique features of the 12 +K-isomer in 174W, which can possess a non-pure intrinsic configuration and/or can be characterised by values of the intrinsic quadrupole moment Q and the rotational g factor gR significantly different with respect to the majority of K-isomers at mass A≈ 180.
g factor of the 12 + K-isomer in 174 W
Giaz A.;
2020-01-01
Abstract
The g factor of the 12 +K-isomer in 174W has been measured by means of the time-differential perturbed angular distribution technique as g(12 +) = + 0.304 (11). In addition, the half-life of the isomer has been remeasured as T1 / 2(12 +) = 124 (8) ns, in agreement with the literature value and confirming the anomalous hindrance F of the E2 transition to the 10 + level of the ground state band with respect to the γ-tunnelling model prediction. The measured g factor has been compared with estimates based on experimental g factors from odd-mass isotopes in the same mass region and with Nilsson model calculations. The results establish unique features of the 12 +K-isomer in 174W, which can possess a non-pure intrinsic configuration and/or can be characterised by values of the intrinsic quadrupole moment Q and the rotational g factor gR significantly different with respect to the majority of K-isomers at mass A≈ 180.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.