nuclear moments
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2021 ◽  
Vol 127 (25) ◽  
Author(s):  
S. G. Porsev ◽  
M. S. Safronova ◽  
M. G. Kozlov

2020 ◽  
Vol 102 (5) ◽  
Author(s):  
A. Kanellakopoulos ◽  
X. F. Yang ◽  
M. L. Bissell ◽  
M. L. Reitsma ◽  
S. W. Bai ◽  
...  
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2020 ◽  
Vol 101 (7) ◽  
Author(s):  
V. V. Flambaum ◽  
H. B. Tran Tan ◽  
D. Budker ◽  
A. Wickenbrock
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2018 ◽  
Vol 782 ◽  
pp. 619-626 ◽  
Author(s):  
Z.Y. Xu ◽  
H. Heylen ◽  
K. Asahi ◽  
F. Boulay ◽  
J.M. Daugas ◽  
...  

2016 ◽  
Vol 115 (6) ◽  
pp. 62002 ◽  
Author(s):  
A. S. Fenta ◽  
S. Pallada ◽  
J. G. Correia ◽  
M. Stachura ◽  
K. Johnston ◽  
...  
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2016 ◽  
Vol 25 (03) ◽  
pp. 1650022 ◽  
Author(s):  
M. S. Nadirbekov ◽  
N. Minkov ◽  
M. Strecker ◽  
W. Scheid

In this work, we examine the possibility to describe yrast positive- and negative-parity excitations of deformed even–even nuclei through a collective rotation model in which the nuclear surface is characterized by triaxial quadrupole and octupole deformations. The nuclear moments of inertia are expressed as sums of quadrupole and octupole parts. By assuming an adiabatic separation of rotation and vibration degrees of freedom, we suppose that the structure of the positive- and negative-parity bands may be determined by the triaxial-rigid-rotor motion of the nucleus. By diagonalizing the Hamiltonian in a symmetrized rotor basis with embedded parity, we obtain a model description for the yrast positive- and negative-parity bands in several actinide nuclei. We show that the energy displacement between the opposite-parity sequences can be explained as the result of the quadrupole–octupole triaxiality.


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