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The merging of the islands of inversion at N=20 and N=28
The N=20 and N=28 "islands of inversion" are described by large scale shell model calculations with an extension of the interaction sdpf-u that makes it possible to mix configurations with different Nhw or equivalently with different number of particles promoted from the sd-shell to the pf...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevC.90.014302 http://cds.cern.ch/record/1603614 |
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author | Caurier, Etienne Nowacki, Frederic Poves, Alfredo |
author_facet | Caurier, Etienne Nowacki, Frederic Poves, Alfredo |
author_sort | Caurier, Etienne |
collection | CERN |
description | The N=20 and N=28 "islands of inversion" are described by large scale shell model calculations with an extension of the interaction sdpf-u that makes it possible to mix configurations with different Nhw or equivalently with different number of particles promoted from the sd-shell to the pf-shell. It allows to connect the classical sd-shell calculations below N=18 with the sd(protons)-pf(neutrons) calculations beyond N=24-26, for all the isotopes from Oxygen to Calcium, using the same interaction. For some isotopes this range contains all the nuclei between the proton and the neutron drip lines and includes the N=20 and N=28 islands of inversion. We shall pay particular attention to the properties of the states at fix Nhw which turn out to be the real protagonists of the physics at N=20. The existence of islands of inversion/deformation will be explained as the result of the competition between the spherical mean field which favors the 0hw configurations and the nuclear correlations which favor the deformed Nhw configurations. The Magnesium chain is exceptional because in it, the N=20 and N=28 "islands of inversion" merge, enclosing all the isotopes between N=19 and N=30. Indeed, this would be also the case for the Neon and Sodium chains if their drip lines would reach N=28. |
id | cern-1603614 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-16036142021-07-16T18:15:22Zdoi:10.1103/PhysRevC.90.014302http://cds.cern.ch/record/1603614engCaurier, EtienneNowacki, FredericPoves, AlfredoThe merging of the islands of inversion at N=20 and N=28Nuclear Physics - TheoryThe N=20 and N=28 "islands of inversion" are described by large scale shell model calculations with an extension of the interaction sdpf-u that makes it possible to mix configurations with different Nhw or equivalently with different number of particles promoted from the sd-shell to the pf-shell. It allows to connect the classical sd-shell calculations below N=18 with the sd(protons)-pf(neutrons) calculations beyond N=24-26, for all the isotopes from Oxygen to Calcium, using the same interaction. For some isotopes this range contains all the nuclei between the proton and the neutron drip lines and includes the N=20 and N=28 islands of inversion. We shall pay particular attention to the properties of the states at fix Nhw which turn out to be the real protagonists of the physics at N=20. The existence of islands of inversion/deformation will be explained as the result of the competition between the spherical mean field which favors the 0hw configurations and the nuclear correlations which favor the deformed Nhw configurations. The Magnesium chain is exceptional because in it, the N=20 and N=28 "islands of inversion" merge, enclosing all the isotopes between N=19 and N=30. Indeed, this would be also the case for the Neon and Sodium chains if their drip lines would reach N=28.The $N=20$ and $N=28$ ``islands of inversion'' are described by large scale shell model calculations with an extension of the interaction SDPF-U that makes it possible to mix configurations with different $\mathrm{N}$\hbar${}$\omega${}$ or equivalently with different numbers of particles promoted from the $sd$ shell to the $pf$ shell. It allows to connect the classical $sd$-shell calculations below $N=18$ with the $sd$ (protons)-$pf$ (neutrons) calculations beyond $N=24\char21{}26$, for all the isotopes from oxygen to sulfur, using the same interaction. For some isotopes this range contains all the nuclei between the proton and the neutron drip lines and includes the $N=20$ and $N=28$ islands of inversion. We pay particular attention to the properties of the states at fixed $\mathrm{N}$\hbar${}$\omega${}$ which turn out to be the real protagonists of the physics at $N=20$. The existence of islands of inversion or deformation are explained as the result of the competition between the spherical mean field which favors the $0$\hbar${}$\omega${}$ configurations and the nuclear correlations which favor the deformed $N$\hbar${}$\omega${}$ configurations. The magnesium chain is exceptional because in it the $N=20$ and $N=28$ islands of inversion merge, enclosing all the isotopes between $N=19$ and $N=30$. Indeed, this would be also the case for the neon and sodium chains if their drip lines would reach $N=28$.The N=20 and N=28 "islands of inversion" are described by large scale shell model calculations with an extension of the interaction sdpf-u that makes it possible to mix configurations with different Nhw or equivalently with different number of particles promoted from the sd-shell to the pf-shell. It allows to connect the classical sd-shell calculations below N=18 with the sd(protons)-pf(neutrons) calculations beyond N=24-26, for all the isotopes from Oxygen to Calcium, using the same interaction. For some isotopes this range contains all the nuclei between the proton and the neutron drip lines and includes the N=20 and N=28 islands of inversion. We shall pay particular attention to the properties of the states at fix Nhw which turn out to be the real protagonists of the physics at N=20. The existence of islands of inversion/deformation will be explained as the result of the competition between the spherical mean field which favors the 0hw configurations and the nuclear correlations which favor the deformed Nhw configurations. The Magnesium chain is exceptional because in it, the N=20 and N=28 "islands of inversion" merge, enclosing all the isotopes between N=19 and N=30. Indeed, this would be also the case for the Neon and Sodium chains if their drip lines would reach N=28.arXiv:1309.6955oai:cds.cern.ch:16036142013-09-26 |
spellingShingle | Nuclear Physics - Theory Caurier, Etienne Nowacki, Frederic Poves, Alfredo The merging of the islands of inversion at N=20 and N=28 |
title | The merging of the islands of inversion at N=20 and N=28 |
title_full | The merging of the islands of inversion at N=20 and N=28 |
title_fullStr | The merging of the islands of inversion at N=20 and N=28 |
title_full_unstemmed | The merging of the islands of inversion at N=20 and N=28 |
title_short | The merging of the islands of inversion at N=20 and N=28 |
title_sort | merging of the islands of inversion at n=20 and n=28 |
topic | Nuclear Physics - Theory |
url | https://dx.doi.org/10.1103/PhysRevC.90.014302 http://cds.cern.ch/record/1603614 |
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