Reduced transition probabilities of vibrational states inGd154−160andHf176−180

1977 ◽  
Vol 15 (5) ◽  
pp. 1671-1678 ◽  
Author(s):  
R. M. Ronningen ◽  
J. H. Hamilton ◽  
A. V. Ramayya ◽  
L. Varnell ◽  
G. Garcia-Bermudez ◽  
...  
1982 ◽  
Vol 26 (1) ◽  
pp. 97-106 ◽  
Author(s):  
R. M. Ronningen ◽  
R. S. Grantham ◽  
J. H. Hamilton ◽  
R. B. Piercey ◽  
A. V. Ramayya ◽  
...  

2018 ◽  
Vol 178 ◽  
pp. 02028 ◽  
Author(s):  
Erin E. Peters ◽  
Timothy J. Ross ◽  
Benjamin P. Crider ◽  
Steven W. Yates

The stable isotopes of xenon, which have attracted interest for a number of reasons, span a transitional region that evolves from γ-soft structures for the lighter mass isotopes to nearly spherical 136Xe with a closed neutron shell. The nature of this transition, which is gradual, is not well understood. To provide detailed spectroscopic information on the Xe isotopes, we have studied 130,132,134,136Xe at the University of Kentucky Accelerator Laboratory using inelastic neutron scattering and γ-ray detection. These measurements yielded γ-ray angular distributions, branching ratios, multipole mixing ratios, and level lifetimes (from the Doppler-shift attenuation method), which allowed the determination of reduced transition probabilities and provided insight into the structure of these nuclei.


2005 ◽  
Vol 25 (S1) ◽  
pp. 409-413 ◽  
Author(s):  
K. Yamada ◽  
T. Motobayashi ◽  
N. Aoi ◽  
H. Baba ◽  
K. Demichi ◽  
...  

2016 ◽  
Vol 94 (4) ◽  
Author(s):  
T. Grahn ◽  
S. Stolze ◽  
D. T. Joss ◽  
R. D. Page ◽  
B. Sayğı ◽  
...  

2014 ◽  
Vol 23 (04) ◽  
pp. 1450020
Author(s):  
Deepti Sharma ◽  
Preeti Verma ◽  
Suram Singh ◽  
Arun Bharti ◽  
S. K. Khosa

Negative parity energy states in 121–131 La have been studied using Projected Shell Model (PSM). Some nuclear structure properties like yrast spectra, back-bending in moment of inertia, reduced transition probabilities and band diagrams have been described. The experimental feature of the co-existence of prolate–oblate shapes in 125–131 La isotopes has been satisfactorily explained by PSM results. Comparison of the theoretical data with their experimental counterparts has also been made. From the calculations, it is found that the yrast states arise because of multi-quasiparticle states.


1998 ◽  
Vol 422 (1-4) ◽  
pp. 13-18 ◽  
Author(s):  
A.A. Adams ◽  
G.E. Mitchell ◽  
J.F. Shriner, Jr

2006 ◽  
Vol 15 (07) ◽  
pp. 1531-1540 ◽  
Author(s):  
D. TONEV ◽  
P. PETKOV ◽  
D. L. BALABANSKI ◽  
G. DE ANGELIS ◽  
A. GADEA ◽  
...  

Lifetimes of exited states in 134 Pr were measured be means of the recoil distance Doppler-shift and Doppler-shift attenuation techniques. The experiments were performed at IReS, Strasbourg using the EUROBALL IV spectrometer, in conjunction with the inner BGO ball and the Cologne coincidence plunger apparatus. Exited states in 134 Pr were populated in the fusion-evaporation reaction 119 Sn (19 F , 4 n )134 Pr . Reduced transition probabilities in 134 Pr are compared to the predictions of the two quasiparticle+triaxial rotor and interacting boson fermion-fermion models. The experimental results do not support the presence of static chirality in 134 Pr underlying the importance of shape fluctuations. Only within a dynamical context the presence of intrinsic chirality in 134 Pr can be supported.


1979 ◽  
Vol 57 (8) ◽  
pp. 1196-1203 ◽  
Author(s):  
V. U. Patil ◽  
R. G. Kulkarni

Low-lying negative parity levels in 45Sc were Coulomb excited with 2.5 to 3.5 MeV protons and 4 to 5 MeV 4He ions to test the weak coupling core-excitation model. A Ge(Li) detector was used to measure the gamma-ray yields. The 543, 976, 1408, and 1662 keV levels in 45Sc were Coulomb excited for the first time. Gamma-ray angular distributions were measured at 3.0 MeV proton energy in deducing multipole mixing ratios and spin values. Energy level measurements (in units of kiloelectronvolts) and spin values obtained are as follows: 976, 5/2, 7/2 and 1408, 7/2. The E2 and M1 reduced transition probabilities were determined for the six states. The 376, 720, 1237, 1408, and 1662 keV levels have properties consistent with the interpretation of coupling a 1f7/2 proton to the first 2+ core state.


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