Studying chirality in a ~ 100, 130 and 190 mass regions

Chirality is a nuclear symmetry which is suggested to occur in nuclei when the total angular momentum of the system has an aplanar orientation [Fra97, Fra01]. It can occur for nuclei with triaxial shape, which have valence protons and neutrons with predominantly particle and hole nature. It is expec...

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Main Author: Shirinda, Obed
Format: Others
Language:English
Published: 2011
Subjects:
Online Access:http://etd.uwc.ac.za/index.php?module=etd&action=viewtitle&id=gen8Srv25Nme4_8742_1319096308
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spelling ndltd-UNWC-oai-UWC_ETD-http%3A%2F%2Fetd.uwc.ac.za%2Findex.php%3Fmodule%3Detd%26action%3Dviewtitle%26id%3Dgen8Srv25Nme4_8742_13190963082013-01-08T12:43:11Z Studying chirality in a ~ 100, 130 and 190 mass regions Shirinda, Obed Quasiparticle-hole configuration Degenerate DI = 1 rotational band Excitation energies Alignment Angular momenta Electromagnetic transitions B(M1) staggering Aplanar rotation Chirality • Two-quasiparticle-plus-triaxial-rotor model. Chirality is a nuclear symmetry which is suggested to occur in nuclei when the total angular momentum of the system has an aplanar orientation [Fra97, Fra01]. It can occur for nuclei with triaxial shape, which have valence protons and neutrons with predominantly particle and hole nature. It is expected that the angular momenta of an odd particle and an odd hole (both occupying high-j orbitals) are aligned predominantly along the short and the long axes of the nucleus respectively, whereas the collective rotation occurs predominantly around the intermediate axis of a triaxially deformed nucleus in order to minimize the total energy of the system. Such symmetry is expected to be exhibited by a pair of degenerate DI = 1 rotational bands, i.e. all properties of the partner bands should be identical. The results suggested that spin independence of the energy staggering parameter S(I ) within two-quasiparticle chiral bands (previously suggested a fingerprint of chirality) is found only if the Coriolis interaction can be completely neglected. However, if the configuration is nonrestricted, the Coriolis interaction is often strong enough to create considerable energy staggering. It was also found that staggering in the intra- and inter-band B(M1) reduced transition probabilities (proposed as another fingerprint of chirality) may be a result of effects other than strongly broken chirality. Therefore, the use of the B(M1) staggering as a fingerprint of strongly broken chiral symmetry seems rather risky, in particular if the phase of the staggering is not checked. 2011 Thesis and dissertation Pdf http://etd.uwc.ac.za/index.php?module=etd&action=viewtitle&id=gen8Srv25Nme4_8742_1319096308 English ZA Copyright: University of the Western Cape
collection NDLTD
language English
format Others
sources NDLTD
topic Quasiparticle-hole configuration
Degenerate DI = 1 rotational band
Excitation energies
Alignment
Angular momenta
Electromagnetic transitions
B(M1) staggering
Aplanar rotation
Chirality
• Two-quasiparticle-plus-triaxial-rotor model.
spellingShingle Quasiparticle-hole configuration
Degenerate DI = 1 rotational band
Excitation energies
Alignment
Angular momenta
Electromagnetic transitions
B(M1) staggering
Aplanar rotation
Chirality
• Two-quasiparticle-plus-triaxial-rotor model.
Shirinda, Obed
Studying chirality in a ~ 100, 130 and 190 mass regions
description Chirality is a nuclear symmetry which is suggested to occur in nuclei when the total angular momentum of the system has an aplanar orientation [Fra97, Fra01]. It can occur for nuclei with triaxial shape, which have valence protons and neutrons with predominantly particle and hole nature. It is expected that the angular momenta of an odd particle and an odd hole (both occupying high-j orbitals) are aligned predominantly along the short and the long axes of the nucleus respectively, whereas the collective rotation occurs predominantly around the intermediate axis of a triaxially deformed nucleus in order to minimize the total energy of the system. Such symmetry is expected to be exhibited by a pair of degenerate DI = 1 rotational bands, i.e. all properties of the partner bands should be identical. The results suggested that spin independence of the energy staggering parameter S(I ) within two-quasiparticle chiral bands (previously suggested a fingerprint of chirality) is found only if the Coriolis interaction can be completely neglected. However, if the configuration is nonrestricted, the Coriolis interaction is often strong enough to create considerable energy staggering. It was also found that staggering in the intra- and inter-band B(M1) reduced transition probabilities (proposed as another fingerprint of chirality) may be a result of effects other than strongly broken chirality. Therefore, the use of the B(M1) staggering as a fingerprint of strongly broken chiral symmetry seems rather risky, in particular if the phase of the staggering is not checked.
author Shirinda, Obed
author_facet Shirinda, Obed
author_sort Shirinda, Obed
title Studying chirality in a ~ 100, 130 and 190 mass regions
title_short Studying chirality in a ~ 100, 130 and 190 mass regions
title_full Studying chirality in a ~ 100, 130 and 190 mass regions
title_fullStr Studying chirality in a ~ 100, 130 and 190 mass regions
title_full_unstemmed Studying chirality in a ~ 100, 130 and 190 mass regions
title_sort studying chirality in a ~ 100, 130 and 190 mass regions
publishDate 2011
url http://etd.uwc.ac.za/index.php?module=etd&action=viewtitle&id=gen8Srv25Nme4_8742_1319096308
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