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Relativistic Chiral Mean Field Model for Finite Nuclei
Pion is important in Nuclear Physics. Yukawa introduced pion as a mediator of nucleon-nucleon interaction in 1934 [1]. However, Nuclear Physics started by shell model with strong spin-orbit interaction in 1949 by Meyer and Jensen. The shell model is a phenomenological model and it has to be explaine...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2010
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/1249543 |
_version_ | 1780919586502213632 |
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author | Toki, H Ikeda, K Ogawa, Y Hu, J Myo, T |
author_facet | Toki, H Ikeda, K Ogawa, Y Hu, J Myo, T |
author_sort | Toki, H |
collection | CERN |
description | Pion is important in Nuclear Physics. Yukawa introduced pion as a mediator of nucleon-nucleon interaction in 1934 [1]. However, Nuclear Physics started by shell model with strong spin-orbit interaction in 1949 by Meyer and Jensen. The shell model is a phenomenological model and it has to be explained from more basic dynamics by explicitly using pion. The pion had not played the central role in nuclear physics until recent years. In this paper, we would like to discuss the recent development on the role of pion in nuclei. |
id | cern-1249543 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2010 |
record_format | invenio |
spelling | cern-12495432019-09-30T06:29:59Zhttp://cds.cern.ch/record/1249543engToki, HIkeda, KOgawa, YHu, JMyo, TRelativistic Chiral Mean Field Model for Finite NucleiXXPion is important in Nuclear Physics. Yukawa introduced pion as a mediator of nucleon-nucleon interaction in 1934 [1]. However, Nuclear Physics started by shell model with strong spin-orbit interaction in 1949 by Meyer and Jensen. The shell model is a phenomenological model and it has to be explained from more basic dynamics by explicitly using pion. The pion had not played the central role in nuclear physics until recent years. In this paper, we would like to discuss the recent development on the role of pion in nuclei.oai:cds.cern.ch:12495432010 |
spellingShingle | XX Toki, H Ikeda, K Ogawa, Y Hu, J Myo, T Relativistic Chiral Mean Field Model for Finite Nuclei |
title | Relativistic Chiral Mean Field Model for Finite Nuclei |
title_full | Relativistic Chiral Mean Field Model for Finite Nuclei |
title_fullStr | Relativistic Chiral Mean Field Model for Finite Nuclei |
title_full_unstemmed | Relativistic Chiral Mean Field Model for Finite Nuclei |
title_short | Relativistic Chiral Mean Field Model for Finite Nuclei |
title_sort | relativistic chiral mean field model for finite nuclei |
topic | XX |
url | http://cds.cern.ch/record/1249543 |
work_keys_str_mv | AT tokih relativisticchiralmeanfieldmodelforfinitenuclei AT ikedak relativisticchiralmeanfieldmodelforfinitenuclei AT ogaway relativisticchiralmeanfieldmodelforfinitenuclei AT huj relativisticchiralmeanfieldmodelforfinitenuclei AT myot relativisticchiralmeanfieldmodelforfinitenuclei |