Nuclear structure effects on heavy-ion reactions with microscopic theory

The self-consistent mean-field Hartree–Fock (HF) theory, both static and time-dependent (TDHF) versions, is used to study static and dynamic properties of fusion reactions between even 40–54Ca isotopes and 116Sn. The bare nucleus-nucleus potential, calculated with the frozen HF approach, is affected...

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Main Authors: Vo-Phuoc K., Simenel C., Simpson E. C.
Format: Article
Language:English
Published: EDP Sciences 2016-01-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/201612303001
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spelling doaj-0f6213ba941f4155a227a2d8f8599ecd2021-08-02T07:44:41ZengEDP SciencesEPJ Web of Conferences2100-014X2016-01-011230300110.1051/epjconf/201612303001epjconf_hias2016_03001Nuclear structure effects on heavy-ion reactions with microscopic theoryVo-Phuoc K.0Simenel C.1Simpson E. C.2Department of Nuclear Physics, Research School of Physics and Engineering, Australian National UniversityDepartment of Nuclear Physics, Research School of Physics and Engineering, Australian National UniversityDepartment of Nuclear Physics, Research School of Physics and Engineering, Australian National UniversityThe self-consistent mean-field Hartree–Fock (HF) theory, both static and time-dependent (TDHF) versions, is used to study static and dynamic properties of fusion reactions between even 40–54Ca isotopes and 116Sn. The bare nucleus-nucleus potential, calculated with the frozen HF approach, is affected by the groundstate density of the nuclei. However, once dynamical effects are included, as in TDHF, the static effects on the barrier are essentially washed out. Dynamic properties of the nuclei, including low-lying vibrational modes, are calculated with TDHF and selectively used in coupled-channels calculations to identify which modes have the most effect on the TDHF fusion threshold. Vibrations cannot fully explain the difference between the static HF and TDHF fusion barriers trend so other dynamical effects such as transfer are considered.http://dx.doi.org/10.1051/epjconf/201612303001
collection DOAJ
language English
format Article
sources DOAJ
author Vo-Phuoc K.
Simenel C.
Simpson E. C.
spellingShingle Vo-Phuoc K.
Simenel C.
Simpson E. C.
Nuclear structure effects on heavy-ion reactions with microscopic theory
EPJ Web of Conferences
author_facet Vo-Phuoc K.
Simenel C.
Simpson E. C.
author_sort Vo-Phuoc K.
title Nuclear structure effects on heavy-ion reactions with microscopic theory
title_short Nuclear structure effects on heavy-ion reactions with microscopic theory
title_full Nuclear structure effects on heavy-ion reactions with microscopic theory
title_fullStr Nuclear structure effects on heavy-ion reactions with microscopic theory
title_full_unstemmed Nuclear structure effects on heavy-ion reactions with microscopic theory
title_sort nuclear structure effects on heavy-ion reactions with microscopic theory
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2016-01-01
description The self-consistent mean-field Hartree–Fock (HF) theory, both static and time-dependent (TDHF) versions, is used to study static and dynamic properties of fusion reactions between even 40–54Ca isotopes and 116Sn. The bare nucleus-nucleus potential, calculated with the frozen HF approach, is affected by the groundstate density of the nuclei. However, once dynamical effects are included, as in TDHF, the static effects on the barrier are essentially washed out. Dynamic properties of the nuclei, including low-lying vibrational modes, are calculated with TDHF and selectively used in coupled-channels calculations to identify which modes have the most effect on the TDHF fusion threshold. Vibrations cannot fully explain the difference between the static HF and TDHF fusion barriers trend so other dynamical effects such as transfer are considered.
url http://dx.doi.org/10.1051/epjconf/201612303001
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AT simenelc nuclearstructureeffectsonheavyionreactionswithmicroscopictheory
AT simpsonec nuclearstructureeffectsonheavyionreactionswithmicroscopictheory
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