2020
DOI: 10.1103/revmodphys.92.015002
|View full text |Cite
|
Sign up to set email alerts
|

Evolution of shell structure in exotic nuclei

Abstract: The atomic nucleus is a quantum many-body system whose constituent nucleons (protons and neutrons) are subject to complex nucleon-nucleon interactions that include spin-and isospin-dependent components. For stable nuclei, already several decades ago, emerging seemingly regular patterns in some observables could be described successfully within a shell-model picture that results in particularly stable nuclei at certain magic fillings of the shells with protons and/or neutrons: N,Z = 8, 20, 28, 50, 82, 126. Howe… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

29
327
2
1

Year Published

2020
2020
2022
2022

Publication Types

Select...
5
3
1

Relationship

1
8

Authors

Journals

citations
Cited by 353 publications
(359 citation statements)
references
References 351 publications
(355 reference statements)
29
327
2
1
Order By: Relevance
“…1; Garcia-Ramos and Heyde 2019), and we also include it in the same column. Even though the magic numbers may change in neutron-rich nuclei when the number of neutrons is much larger than the number of protons (Steppenbeck 2013;Otsuka 2020), in this paper we consider only those nuclei which are close to the beta-stability line and do not consider such effect. Though the heaviest element discovered so far is Oganessson (Z=118), the proton magic number after Z=82 is currently unknown.…”
Section: Nuclear Periodic Tablementioning
confidence: 99%
“…1; Garcia-Ramos and Heyde 2019), and we also include it in the same column. Even though the magic numbers may change in neutron-rich nuclei when the number of neutrons is much larger than the number of protons (Steppenbeck 2013;Otsuka 2020), in this paper we consider only those nuclei which are close to the beta-stability line and do not consider such effect. Though the heaviest element discovered so far is Oganessson (Z=118), the proton magic number after Z=82 is currently unknown.…”
Section: Nuclear Periodic Tablementioning
confidence: 99%
“…(a) Neutron effective single-particle energies (ESPEs) for N=8 isotones obtained by using monopoles of SFO [9] and PSDMK2 [12]. (b) Energy levels of 12 Be obtained by shell-model calculations with SFO (6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16) and PSDMK2 as well as experimental values [14].…”
Section: Melting Of N=8 Magicity and New Shell-model Hamiltoniansmentioning
confidence: 99%
“…We show in Fig. 1(b) the case for SFO (6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16), where the p-shell part is taken to be TBE(6-16) interaction instead of POT(8-16) interaction [5]. Calculated B(E2) value is 8.1 fm 4 for the effective charges e p =1.2 and e n =0.3, while the experimental value is 6.4-7.6 fm 4 [14].…”
Section: Melting Of N=8 Magicity and New Shell-model Hamiltoniansmentioning
confidence: 99%
“…In the light-and medium-mass regions, structural changes have been evidenced for nuclei with a large excess of neutrons, leading to the breakdown of the traditional magic numbers and the appearance of new ones. These findings have driven a great theoretical effort to understand the microscopic mechanism underlying the shell evolution, with special attention to the role of the different components of the nuclear force (see, for instance, [5]). It is of great interest to verify if peculiar properties, as those observed in lighter nuclei, may be also observed in the 132 Sn region.…”
Section: Introductionmentioning
confidence: 99%