Calculation of the Positive Parity Yrast Bands of 190–198Hg Nuclei

2017 ◽  
Vol 62 (8) ◽  
pp. 653-660 ◽  
Author(s):  
K.A. Hussain ◽  
F.I. Sharrad ◽  
◽  
M.K. Mohsin ◽  
◽  
...  
Keyword(s):  
2014 ◽  
Vol 89 (7) ◽  
pp. 713-722 ◽  
Author(s):  
S. Sadiq ◽  
D. Ram ◽  
R. Devi ◽  
S. K. Khosa
Keyword(s):  

2018 ◽  
Author(s):  
Rakesh K. Pandit ◽  
Shivali Sharma ◽  
Rani Devi ◽  
S. K. Khosa
Keyword(s):  

Pramana ◽  
2013 ◽  
Vol 80 (6) ◽  
pp. 953-970 ◽  
Author(s):  
DAYA RAM ◽  
RANI DEVI ◽  
S K KHOSA

2019 ◽  
Vol 1279 ◽  
pp. 012021
Author(s):  
Mahdi A. Mahdi ◽  
Fahmi Sh. Radhi ◽  
Huda H. Kassim ◽  
Mushtaq AbedAlJubbori ◽  
Fadhil I. Sharrad
Keyword(s):  

2008 ◽  
Vol 17 (supp01) ◽  
pp. 304-317
Author(s):  
Y. M. ZHAO

In this paper we review regularities of low-lying states for many-body systems, in particular, atomic nuclei, under random interactions. We shall discuss the famous problem of spin zero ground state dominance, positive parity dominance, collective motion, odd-even staggering, average energies, etc., in the presence of random interactions.


1984 ◽  
Vol 37 (1) ◽  
pp. 17 ◽  
Author(s):  
FC Barker

On the basis of a weak-coupling model, adjustments are made to the interactions used in the full shell model calculations of Millener in order to fit the experimental energies of the low-lying negativeparity levels of 16N and of the low-lying positive-parity levels of 180 and 190 . The predicted energies of the low-lying negative-parity levels of 17N then agree better with experiment, while those for 18N lead to suggested spin assignments for the observed levels.


1977 ◽  
Vol 275 (1) ◽  
pp. 61-75 ◽  
Author(s):  
W.D. Teeters ◽  
D. Kurath
Keyword(s):  

2006 ◽  
Vol 21 (31n33) ◽  
pp. 2373-2382 ◽  
Author(s):  
Taiichi YAMADA ◽  
Hisashi HORIUCHI ◽  
Peter SCHUCK

The spin-orbit splittings of 13 C and 13 N corresponding to the ground state and second 0+ state (Hoyle state) in 12 C are investigated within a 12 C +N model. The agreement of the calculated results with experiments suggests that the [Formula: see text] and [Formula: see text] states around Ex = 9 ~ 10 MeV in 13 C and 13 N can be interpreted as the spin-orbit partner with the [Formula: see text] configuration. We also discuss the positive parity states (including [Formula: see text]) of 13 C and 13 N around the [Formula: see text] threshold, indicating to have the configuration of the Hoyle state in 12 C plus a valence nucleon in sd shell.


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