2008
DOI: 10.1103/physrevc.77.024308
|View full text |Cite
|
Sign up to set email alerts
|

Projected shell model study of neutron-rich deformed isotopes of Sr and Zr

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
7
0

Year Published

2012
2012
2023
2023

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 22 publications
(7 citation statements)
references
References 47 publications
0
7
0
Order By: Relevance
“…Two main mechanisms based on shell models and mean-field approaches were proposed to explain the sudden onset of large nuclear collectivity at N = 60, namely, a strong isoscalar proton-neutron interaction between particles occupying the g 9/2 -g 7/2 spin-orbit partners [12], and the occupation of low-K components of the h 11/2 neutron orbit [26,27] respectively. Besides these two factors, the simultaneous polarization of 2p 1/2 , 2p 3/2 , and 1f 5/2 proton orbits as one goes from 96 Sr to 98 Sr and from 98 Zr to 100 Zr was pointed out to be the the major factor in the more recent projected shell model study [28]. However, in most of the previous studies for nuclear low-lying states with, for instance the (projected) shell model, either a phenomenological effective interaction or effective charges for neutrons and protons defined within a specific valence space was introduced.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Two main mechanisms based on shell models and mean-field approaches were proposed to explain the sudden onset of large nuclear collectivity at N = 60, namely, a strong isoscalar proton-neutron interaction between particles occupying the g 9/2 -g 7/2 spin-orbit partners [12], and the occupation of low-K components of the h 11/2 neutron orbit [26,27] respectively. Besides these two factors, the simultaneous polarization of 2p 1/2 , 2p 3/2 , and 1f 5/2 proton orbits as one goes from 96 Sr to 98 Sr and from 98 Zr to 100 Zr was pointed out to be the the major factor in the more recent projected shell model study [28]. However, in most of the previous studies for nuclear low-lying states with, for instance the (projected) shell model, either a phenomenological effective interaction or effective charges for neutrons and protons defined within a specific valence space was introduced.…”
Section: Introductionmentioning
confidence: 99%
“…Besides these two factors, the simultaneous polarization of 2p 1/2 , 2p 3/2 , and 1f 5/2 proton orbits as one goes from 96 Sr to 98 Sr and from 98 Zr to 100 Zr was pointed out to be the the major factor in the more recent projected shell model study [28]. However, in most of the previous studies for nuclear low-lying states with, for instance the (projected) shell model, either a phenomenological effective interaction or effective charges for neutrons and protons defined within a specific valence space was introduced.…”
Section: Introductionmentioning
confidence: 99%
“…On the theoretical side, the shape evolution around N = 60 has been studied extensively with various theoretical models, including the phenomenological models [15,16,17,18,19,20,21,22], the interacting boson model [23], the modern shell model [24] and the self-consistent mean-field models with the Skyrme force [25,26,27], the Gogny force [28,29,30] as well as the effective relativistic Lagrangian [31]. Most of these models have shown the increasing of deformations up to N = 60 and indeed found the competing prolate and oblate minima.…”
Section: Introductionmentioning
confidence: 99%
“…This was first ascribed to the neutron-proton interactions of the spatially-overlapping spin-orbit partner orbits, πg 7/2 and νg 9/2 [2]. However, more recent calculations [3] and g-factor [4] measurements have underlined the importance of core polarisation and the influence of the low-Ω νh 11/2 orbitals.…”
Section: Introductionmentioning
confidence: 99%