scholarly journals Symplectic no-core shell-model approach to intermediate-mass nuclei

2014 ◽  
Vol 89 (3) ◽  
Author(s):  
G. K. Tobin ◽  
M. C. Ferriss ◽  
K. D. Launey ◽  
T. Dytrych ◽  
J. P. Draayer ◽  
...  
2014 ◽  
Vol 24 (6) ◽  
pp. 988-993 ◽  
Author(s):  
M. Srinivas ◽  
Dhaval Modi ◽  
Nimesh Patel ◽  
V. Verma ◽  
K. V. R. Murthy

1987 ◽  
Vol 197 (4) ◽  
pp. 484-488 ◽  
Author(s):  
X. Ji ◽  
M. Vallieres ◽  
P. Halse

2012 ◽  
Vol 387 ◽  
pp. 012016
Author(s):  
T Dytrych ◽  
K D Launey ◽  
J P Draayer ◽  
D Langr

2021 ◽  
Vol 1028 ◽  
pp. 193-198
Author(s):  
Budi Adiperdana ◽  
Nadya Larasati Kartika ◽  
Risdiana

Ising core-shell model was proposed to reconstruct superparamagnetism hysteresis in nano-goethite (α-FeOOH). Core and shell set as antiferromagnetic and paramagnetic state respectively. Core and shell radius varies until the theoretical hysteresis fit with experiment hysteresis. At low temperature, the hysteresis reconstructed nicely with 55% antiferromagnetic core contribution and 45% paramagnetic shell contribution. At high temperature, the core-shell model show unrealistic result compared to the pure paramagnetic state.


2006 ◽  
Vol 73 (6) ◽  
Author(s):  
P. Navrátil ◽  
C. A. Bertulani ◽  
E. Caurier

2014 ◽  
Vol 55 (8-10) ◽  
pp. 857-860 ◽  
Author(s):  
D. Gazda ◽  
J. Mareš ◽  
P. Navrátil ◽  
R. Roth ◽  
R. Wirth

2018 ◽  
Vol 178 ◽  
pp. 02015
Author(s):  
Chong Qi

In this contribution I present systematic calculations on the spectroscopy and electromagnetic transition properties of intermediate-mass and heavy nuclei around 100Sn and 208Pb. We employed the large-scale configuration interaction shell model approach with realistic interactions. Those nuclei are the longest isotopic chains that can be studied by the nuclear shell model. I will show that the yrast spectra of Te isotopes show a vibrational-like equally spaced pattern but the few known E2 transitions show rotational-like behaviour. These kinds of abnormal collective behaviors cannot be reproduced by standard collective models and provide excellent background to study the competition of single-particle and various collective degrees of freedom. Moreover, the calculated B(E2) values for neutron-deficient and heavier Te isotopes show contrasting different behaviours along the yrast line, which may be related to the enhanced neutron-proton correlation when approaching N=50. The deviations between theory and experiment concerning the energies and E2 transition properties of low-lying 0+ and 2+ excited states and isomeric states in those nuclei may provide a constraint on our understanding of nuclear deformation and intruder configuration in that region.


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