Isospin effect of the in-medium nucleon-nucleon cross section in excited nuclear reactions
Using relativistic mean field theory, the neutron and the proton density distribution of 56Ni nuclei could be obtained in the ground state and the excited state. Based on the framework of the quantum molecular dynamics model, the 56Ni nuclei have been simulated in ground state and in the neutron or...
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| Published in | Chinese physics C Vol. 38; no. 5; pp. 33 - 37 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
01.05.2014
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| Subjects | |
| Online Access | Get full text |
| ISSN | 1674-1137 0254-3052 |
| DOI | 10.1088/1674-1137/38/5/054103 |
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| Abstract | Using relativistic mean field theory, the neutron and the proton density distribution of 56Ni nuclei could be obtained in the ground state and the excited state. Based on the framework of the quantum molecular dynamics model, the 56Ni nuclei have been simulated in ground state and in the neutron or proton excited state. We then used the three different states of 56Ni to collide with the 56Ni in the ground state. To discuss the evolution of the nuclear stopping in different reactions, two kinds of different excited nuclear reactions were studied at different reaction energies and at different impact parameters. Studies have shown that the nuclear stopping of an excited nuclear reaction is sensitive to the isospin-dependent in-medium nucleon-nucleon cross section, compared with the response value of the ground state nuclear reaction. So, it is better for the excited nuclei to extract the isospin dependence of nucleon-nucleon cross section information. |
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| AbstractList | Using relativistic mean field theory, the neutron and the proton density distribution of super(56)Ni nuclei could be obtained in the ground state and the excited state. Based on the framework of the quantum molecular dynamics model, the super(56)Ni nuclei have been simulated in ground state and in the neutron or proton excited state. We then used the three different states of super(56)Ni to collide with the super(56)Ni in the ground state. To discuss the evolution of the nuclear stopping in different reactions, two kinds of different excited nuclear reactions were studied at different reaction energies and at different impact parameters. Studies have shown that the nuclear stopping of an excited nuclear reaction is sensitive to the isospin-dependent in-medium nucleon-nucleon cross section, compared with the response value of the ground state nuclear reaction. So, it is better for the excited nuclei to extract the isospin dependence of nucleon-nucleon cross section information. Using relativistic mean field theory, the neutron and the proton density distribution of 56Ni nuclei could be obtained in the ground state and the excited state. Based on the framework of the quantum molecular dynamics model, the 56Ni nuclei have been simulated in ground state and in the neutron or proton excited state. We then used the three different states of 56Ni to collide with the 56Ni in the ground state. To discuss the evolution of the nuclear stopping in different reactions, two kinds of different excited nuclear reactions were studied at different reaction energies and at different impact parameters. Studies have shown that the nuclear stopping of an excited nuclear reaction is sensitive to the isospin-dependent in-medium nucleon-nucleon cross section, compared with the response value of the ground state nuclear reaction. So, it is better for the excited nuclei to extract the isospin dependence of nucleon-nucleon cross section information. |
| Author | 张傲 郭文军 黄江伟 杨林孟 |
| AuthorAffiliation | College of Science, University of Shanghai for Science and Technology, Shanghai 200093, China Department of Physics and Astronomy, Texas A&M University-Commerce, Commerce, TX 75429, USA |
| Author_xml | – sequence: 1 fullname: 张傲 郭文军 黄江伟 杨林孟 |
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| Cites_doi | 10.1016/S0370-2693(02)02174-3 10.1103/PhysRevC.85.024602 10.1103/PhysRevC.72.064611 10.1103/PhysRevLett.77.3963 10.1016/0370-2693(86)90916-0 10.1103/PhysRev.166.949 10.1016/0375-9474(96)00037-1 10.1088/0031-8949/47/2/004 10.1103/PhysRevC.37.2451 10.1016/0370-1573(91)90094-3 10.1103/PhysRevLett.86.975 10.1103/PhysRevLett.94.032701 10.1103/PhysRevC.55.540 10.1103/PhysRevC.85.017604 10.1103/PhysRevC.58.2283 10.1088/1674-1137/33/10/006 10.1103/PhysRevC.86.034611 10.1103/PhysRevC.85.034601 10.1103/PhysRevC.67.024608 |
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| Notes | Using relativistic mean field theory, the neutron and the proton density distribution of 56Ni nuclei could be obtained in the ground state and the excited state. Based on the framework of the quantum molecular dynamics model, the 56Ni nuclei have been simulated in ground state and in the neutron or proton excited state. We then used the three different states of 56Ni to collide with the 56Ni in the ground state. To discuss the evolution of the nuclear stopping in different reactions, two kinds of different excited nuclear reactions were studied at different reaction energies and at different impact parameters. Studies have shown that the nuclear stopping of an excited nuclear reaction is sensitive to the isospin-dependent in-medium nucleon-nucleon cross section, compared with the response value of the ground state nuclear reaction. So, it is better for the excited nuclei to extract the isospin dependence of nucleon-nucleon cross section information. 11-5641/O4 quantum molecular dynamics, excited state, nuclear stopping, isospin effect ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
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| References | 11 Chen L W (18) 1998; 58 14 15 16 17 Gao Y (13) 2009; 33 19 1 2 3 4 5 6 7 8 9 20 Li B A (10) 1993; 47 Ring P (12) 1996; 37 |
| References_xml | – ident: 19 doi: 10.1016/S0370-2693(02)02174-3 – volume: 37 start-page: 193 issn: 0029-5582 year: 1996 ident: 12 publication-title: Nucl. Phys. – ident: 3 doi: 10.1103/PhysRevC.85.024602 – ident: 5 doi: 10.1103/PhysRevC.72.064611 – ident: 15 doi: 10.1103/PhysRevLett.77.3963 – ident: 16 doi: 10.1016/0370-2693(86)90916-0 – ident: 20 doi: 10.1103/PhysRev.166.949 – ident: 9 doi: 10.1016/0375-9474(96)00037-1 – volume: 47 start-page: 151 issn: 1402-4896 year: 1993 ident: 10 publication-title: Phys. Scr. doi: 10.1088/0031-8949/47/2/004 – ident: 17 doi: 10.1103/PhysRevC.37.2451 – ident: 1 doi: 10.1016/0370-1573(91)90094-3 – ident: 8 doi: 10.1103/PhysRevLett.86.975 – ident: 6 doi: 10.1103/PhysRevLett.94.032701 – ident: 14 doi: 10.1103/PhysRevC.55.540 – ident: 4 doi: 10.1103/PhysRevC.85.017604 – volume: 58 start-page: 2283 issn: 0556-2813 year: 1998 ident: 18 publication-title: Phys. Rev. doi: 10.1103/PhysRevC.58.2283 – volume: 33 start-page: 848 year: 2009 ident: 13 publication-title: Chin. Phys. C (HEP & NP) doi: 10.1088/1674-1137/33/10/006 – ident: 7 doi: 10.1103/PhysRevC.86.034611 – ident: 2 doi: 10.1103/PhysRevC.85.034601 – ident: 11 doi: 10.1103/PhysRevC.67.024608 |
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| Snippet | Using relativistic mean field theory, the neutron and the proton density distribution of 56Ni nuclei could be obtained in the ground state and the excited... Using relativistic mean field theory, the neutron and the proton density distribution of super(56)Ni nuclei could be obtained in the ground state and the... |
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| SubjectTerms | Cross sections Evolution Excitation Ground state Molecular dynamics Nuclear reactions Nuclei Reactions (nuclear) 介质 兴奋 同位旋效应 同位旋相关 核反应 核子碰撞截面 相对论平均场理论 量子分子动力学模型 |
| Title | Isospin effect of the in-medium nucleon-nucleon cross section in excited nuclear reactions |
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