16O + 16O cluster states and their fusion to 32S: A non-monotonic potential description
Non-monotonic (NM) nucleus-nucleus potential families rooted in the Pauli-compliant Energy Density Functional (EDF) theory and especially their behavior at higher energies have been investigated using experimental data for 16O + 16O elastic scattering in the range . At , the 16O + 16O NM potentials...
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Veröffentlicht in: | Europhysics letters 2022-05, Vol.138 (4), p.44002 |
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container_title | Europhysics letters |
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creator | Basak, A. K. Merchant, A. C. Freer, M. Islam, M. Sujan Ramon, Ragib Absar Rahman, M. Mizanur Tariq, A. S. B. Uddin, M. A. Soylu, A. |
description | Non-monotonic (NM) nucleus-nucleus potential families rooted in the Pauli-compliant Energy Density Functional (EDF) theory and especially their behavior at higher energies have been investigated using experimental data for 16O + 16O elastic scattering in the range . At , the 16O + 16O NM potentials in a simple optical model (OM) are found to support five rotational bands of 16O + 16O bound and quasi-molecular states in 32S with the cluster global quantum numbers G = 24, 26, 28, 30 and 32. The lowest band in the experimental spectrum starting at , and having , 2+, 4+, 6+ and 8+, has been located for the first time. In the simple OM, the NM potentials are found to reproduce the experimental 16O + 16O fusion cross-sections in the energy range 12–31 MeV. The present work shows that both the 16O + 16O cluster bands and fusion cross-sections in the Coulomb barrier region can be reproduced using NM potentials. |
doi_str_mv | 10.1209/0295-5075/ac6c48 |
format | Article |
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K. ; Merchant, A. C. ; Freer, M. ; Islam, M. Sujan ; Ramon, Ragib Absar ; Rahman, M. Mizanur ; Tariq, A. S. B. ; Uddin, M. A. ; Soylu, A.</creator><creatorcontrib>Basak, A. K. ; Merchant, A. C. ; Freer, M. ; Islam, M. Sujan ; Ramon, Ragib Absar ; Rahman, M. Mizanur ; Tariq, A. S. B. ; Uddin, M. A. ; Soylu, A.</creatorcontrib><description>Non-monotonic (NM) nucleus-nucleus potential families rooted in the Pauli-compliant Energy Density Functional (EDF) theory and especially their behavior at higher energies have been investigated using experimental data for 16O + 16O elastic scattering in the range . At , the 16O + 16O NM potentials in a simple optical model (OM) are found to support five rotational bands of 16O + 16O bound and quasi-molecular states in 32S with the cluster global quantum numbers G = 24, 26, 28, 30 and 32. The lowest band in the experimental spectrum starting at , and having , 2+, 4+, 6+ and 8+, has been located for the first time. In the simple OM, the NM potentials are found to reproduce the experimental 16O + 16O fusion cross-sections in the energy range 12–31 MeV. 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At , the 16O + 16O NM potentials in a simple optical model (OM) are found to support five rotational bands of 16O + 16O bound and quasi-molecular states in 32S with the cluster global quantum numbers G = 24, 26, 28, 30 and 32. The lowest band in the experimental spectrum starting at , and having , 2+, 4+, 6+ and 8+, has been located for the first time. In the simple OM, the NM potentials are found to reproduce the experimental 16O + 16O fusion cross-sections in the energy range 12–31 MeV. The present work shows that both the 16O + 16O cluster bands and fusion cross-sections in the Coulomb barrier region can be reproduced using NM potentials.</description><subject>Band theory</subject><subject>Clusters</subject><subject>Cross-sections</subject><subject>Elastic scattering</subject><subject>Modulus of elasticity</subject><subject>Quantum numbers</subject><subject>Rotational spectra</subject><subject>Rotational states</subject><issn>0295-5075</issn><issn>1286-4854</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNpFkL1OwzAUhS0EEqWwM1pihFBf_8Vhq6ryI1XqQBemyLUd4arYIXbep8_SJyNREUxnOJ_u1fkQugXyCJRUM0IrUQhSipk20nB1hiZAlSy4EvwcTf7qS3SV0o4QAAVygj5Aro-H--NhSGz2fcquwynr7BLWweL86XyHmz75GHCOmNH3JzzHIYbiK4aYY_AGtzG7kL3eY-uS6XybB_oaXTR6n9zNb07R5nm5WbwWq_XL22K-KrwUtGCM8spoazVwIcARU1lNtZNcWcuA2IZbY3TJyFZtrSkdV8wqqY0WpVRmy6bo7nS27eJ371Kud7HvwvCxZgDDTAqUDtTDifKx_QeA1KO7epRTj3Lqkzv2AysjYsI</recordid><startdate>20220501</startdate><enddate>20220501</enddate><creator>Basak, A. 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A.</au><au>Soylu, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>16O + 16O cluster states and their fusion to 32S: A non-monotonic potential description</atitle><jtitle>Europhysics letters</jtitle><stitle>EPL</stitle><addtitle>EPL</addtitle><date>2022-05-01</date><risdate>2022</risdate><volume>138</volume><issue>4</issue><spage>44002</spage><pages>44002-</pages><issn>0295-5075</issn><eissn>1286-4854</eissn><coden>EULEEJ</coden><abstract>Non-monotonic (NM) nucleus-nucleus potential families rooted in the Pauli-compliant Energy Density Functional (EDF) theory and especially their behavior at higher energies have been investigated using experimental data for 16O + 16O elastic scattering in the range . At , the 16O + 16O NM potentials in a simple optical model (OM) are found to support five rotational bands of 16O + 16O bound and quasi-molecular states in 32S with the cluster global quantum numbers G = 24, 26, 28, 30 and 32. The lowest band in the experimental spectrum starting at , and having , 2+, 4+, 6+ and 8+, has been located for the first time. In the simple OM, the NM potentials are found to reproduce the experimental 16O + 16O fusion cross-sections in the energy range 12–31 MeV. The present work shows that both the 16O + 16O cluster bands and fusion cross-sections in the Coulomb barrier region can be reproduced using NM potentials.</abstract><cop>Les Ulis</cop><pub>EDP Sciences, IOP Publishing and Società Italiana di Fisica</pub><doi>10.1209/0295-5075/ac6c48</doi><tpages>7</tpages></addata></record> |
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subjects | Band theory Clusters Cross-sections Elastic scattering Modulus of elasticity Quantum numbers Rotational spectra Rotational states |
title | 16O + 16O cluster states and their fusion to 32S: A non-monotonic potential description |
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