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Single-Particle Spectrum of Pure Neutron Matter
We have calculated the self-consistent auxiliary potential effects on the binding energy of neutron matter using the Brueckner-Hartree-Fock approach by adopting the Argonne V18 and CD-Bonn potentials. The binding energy with the four different choices for the self-consistent auxiliary potential is d...
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Published in: | Journal of the Physical Society of Japan 2015-03, Vol.84 (3), p.1-1 |
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container_title | Journal of the Physical Society of Japan |
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creator | Gad, Khalaf Mansour, Hesham |
description | We have calculated the self-consistent auxiliary potential effects on the binding energy of neutron matter using the Brueckner-Hartree-Fock approach by adopting the Argonne V18 and CD-Bonn potentials. The binding energy with the four different choices for the self-consistent auxiliary potential is discussed. Also, the binding energy of neutron matter has been computed within the framework of the self-consistent Green's function approach. We also compare the binding energies obtained in this study with those obtained by various microscopic approaches. It is found that the use of the continuous choice tends to give binding energies about 2-4 MeV larger than the gap choice at k... = 1.8 fm... In the case of symmetric nuclear matter this difference is larger. (ProQuest: ... denotes formulae/symbols omitted.) |
doi_str_mv | 10.7566/JPSJ.84.034201 |
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The binding energy with the four different choices for the self-consistent auxiliary potential is discussed. Also, the binding energy of neutron matter has been computed within the framework of the self-consistent Green's function approach. We also compare the binding energies obtained in this study with those obtained by various microscopic approaches. It is found that the use of the continuous choice tends to give binding energies about 2-4 MeV larger than the gap choice at k... = 1.8 fm... In the case of symmetric nuclear matter this difference is larger. 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The binding energy with the four different choices for the self-consistent auxiliary potential is discussed. Also, the binding energy of neutron matter has been computed within the framework of the self-consistent Green's function approach. We also compare the binding energies obtained in this study with those obtained by various microscopic approaches. It is found that the use of the continuous choice tends to give binding energies about 2-4 MeV larger than the gap choice at k... = 1.8 fm... In the case of symmetric nuclear matter this difference is larger. (ProQuest: ... denotes formulae/symbols omitted.)</description><subject>Argon</subject><subject>Binding energy</subject><subject>Binding energy (nuclear)</subject><subject>Cadmium</subject><subject>Comparative analysis</subject><subject>Energy</subject><subject>Mathematical analysis</subject><subject>Microscopy</subject><subject>Neutrons</subject><subject>Nuclear matter</subject><subject>Spectrum analysis</subject><subject>Symbols</subject><subject>Symmetry</subject><issn>0031-9015</issn><issn>1347-4073</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNpdjk1Lw0AUABdRsFavngNevKR9bz_eZo9StFqqBqrnst28SEuaxM3m_1vQk6e5DMMIcYsws4Zovio3q1mhZ6C0BDwTE1Ta5hqsOhcTAIW5AzSX4moYDgDSoNQTMd_s26-G89LHtA8NZ5ueQ4rjMevqrBwjZ288pti12atPieO1uKh9M_DNH6fi8-nxY_Gcr9-XL4uHdd6jppQr2hmSlioGFQwarOuKAuHOyZ2vyAYGWyjviGujwFVAQN5isKBrZOfVVNz_dvvYfY88pO1xPwRuGt9yNw5btOAsSQN0Uu_-qYdujO3pbovkJGhbFKB-AIazUes</recordid><startdate>20150301</startdate><enddate>20150301</enddate><creator>Gad, Khalaf</creator><creator>Mansour, Hesham</creator><general>The Physical Society of Japan</general><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20150301</creationdate><title>Single-Particle Spectrum of Pure Neutron Matter</title><author>Gad, Khalaf ; Mansour, Hesham</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p146t-36b56276de03c5151ffd6c61b92bad67ce0783a96ef5309d0606a71c704f1e9a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Argon</topic><topic>Binding energy</topic><topic>Binding energy (nuclear)</topic><topic>Cadmium</topic><topic>Comparative analysis</topic><topic>Energy</topic><topic>Mathematical analysis</topic><topic>Microscopy</topic><topic>Neutrons</topic><topic>Nuclear matter</topic><topic>Spectrum analysis</topic><topic>Symbols</topic><topic>Symmetry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gad, Khalaf</creatorcontrib><creatorcontrib>Mansour, Hesham</creatorcontrib><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of the Physical Society of Japan</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gad, Khalaf</au><au>Mansour, Hesham</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Single-Particle Spectrum of Pure Neutron Matter</atitle><jtitle>Journal of the Physical Society of Japan</jtitle><date>2015-03-01</date><risdate>2015</risdate><volume>84</volume><issue>3</issue><spage>1</spage><epage>1</epage><pages>1-1</pages><issn>0031-9015</issn><eissn>1347-4073</eissn><abstract>We have calculated the self-consistent auxiliary potential effects on the binding energy of neutron matter using the Brueckner-Hartree-Fock approach by adopting the Argonne V18 and CD-Bonn potentials. The binding energy with the four different choices for the self-consistent auxiliary potential is discussed. Also, the binding energy of neutron matter has been computed within the framework of the self-consistent Green's function approach. We also compare the binding energies obtained in this study with those obtained by various microscopic approaches. It is found that the use of the continuous choice tends to give binding energies about 2-4 MeV larger than the gap choice at k... = 1.8 fm... In the case of symmetric nuclear matter this difference is larger. (ProQuest: ... denotes formulae/symbols omitted.)</abstract><cop>Tokyo</cop><pub>The Physical Society of Japan</pub><doi>10.7566/JPSJ.84.034201</doi><tpages>1</tpages></addata></record> |
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source | American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list) |
subjects | Argon Binding energy Binding energy (nuclear) Cadmium Comparative analysis Energy Mathematical analysis Microscopy Neutrons Nuclear matter Spectrum analysis Symbols Symmetry |
title | Single-Particle Spectrum of Pure Neutron Matter |
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