Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear Theories

We propose the first application of the Cluster Shell Model (CSM) of Della Rocca and Iachello to particle-hole (p-h) states in 8Be. We demonstrate a few essential features of the CSM in 8Be: 1) All predicted p-h states of the CSM, and only the predicted p-h states, are observed near thresholds and u...

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Main Author: Gai Moshe
Format: Article
Language:English
Published: EDP Sciences 2019-01-01
Series:EPJ Web of Conferences
Online Access:https://www.epj-conferences.org/articles/epjconf/pdf/2019/28/epjconf_nsd2019_01019.pdf
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spelling doaj-0f49ddc7a1c54b62a6a8b365c8c2eea02021-08-02T12:04:03ZengEDP SciencesEPJ Web of Conferences2100-014X2019-01-012230101910.1051/epjconf/201922301019epjconf_nsd2019_01019Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear TheoriesGai MosheWe propose the first application of the Cluster Shell Model (CSM) of Della Rocca and Iachello to particle-hole (p-h) states in 8Be. We demonstrate a few essential features of the CSM in 8Be: 1) All predicted p-h states of the CSM, and only the predicted p-h states, are observed near thresholds and up to 19.5 MeV in 8Be. 2) The states are observed in the predicted order, with positive parity states below negative parity states. 3) Some of the p-h states are already known to have the rotational structure predicted for the deformed p-h states. 4) The rotational structures observed at high excitations in the p-h bands in 8Be, resemble the ground state bands of 8Be, 9Be and 9B, with similar moment of inertia. Based on these observations we contemplate new measurements of the spectroscopy of 8Be at energies above 19.5 MeV, where our knowledge of states in 8Be is scarce. We examine the observed B(M1)s and B(E2)s in these nuclei and contemplate a measurement of the B(E2) of the isobaric Analog transition in 8B. We discuss the observed rotational structure in 8Be as a challenge to ab-initio calculations that searched for “emerging rotational structures at high excitations" in beryllium nuclei, and reveal rotational structure at high excitations in 10Be and 12Be but not in 8Be.https://www.epj-conferences.org/articles/epjconf/pdf/2019/28/epjconf_nsd2019_01019.pdf
collection DOAJ
language English
format Article
sources DOAJ
author Gai Moshe
spellingShingle Gai Moshe
Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear Theories
EPJ Web of Conferences
author_facet Gai Moshe
author_sort Gai Moshe
title Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear Theories
title_short Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear Theories
title_full Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear Theories
title_fullStr Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear Theories
title_full_unstemmed Particle-Hole Cluster Shell Model States in 8Be, a Challenge for Ab-Intio Nuclear Theories
title_sort particle-hole cluster shell model states in 8be, a challenge for ab-intio nuclear theories
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2019-01-01
description We propose the first application of the Cluster Shell Model (CSM) of Della Rocca and Iachello to particle-hole (p-h) states in 8Be. We demonstrate a few essential features of the CSM in 8Be: 1) All predicted p-h states of the CSM, and only the predicted p-h states, are observed near thresholds and up to 19.5 MeV in 8Be. 2) The states are observed in the predicted order, with positive parity states below negative parity states. 3) Some of the p-h states are already known to have the rotational structure predicted for the deformed p-h states. 4) The rotational structures observed at high excitations in the p-h bands in 8Be, resemble the ground state bands of 8Be, 9Be and 9B, with similar moment of inertia. Based on these observations we contemplate new measurements of the spectroscopy of 8Be at energies above 19.5 MeV, where our knowledge of states in 8Be is scarce. We examine the observed B(M1)s and B(E2)s in these nuclei and contemplate a measurement of the B(E2) of the isobaric Analog transition in 8B. We discuss the observed rotational structure in 8Be as a challenge to ab-initio calculations that searched for “emerging rotational structures at high excitations" in beryllium nuclei, and reveal rotational structure at high excitations in 10Be and 12Be but not in 8Be.
url https://www.epj-conferences.org/articles/epjconf/pdf/2019/28/epjconf_nsd2019_01019.pdf
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