Spontaneous chiral symmetry breaking in the massless linear sigma model by fermion and boson loop corrections

Tamenaga, Setsuo; Toki, H.; Haga, Akihiro; Ogawa, Yoko

doi:10.1016/j.nuclphysa.2008.07.015

Nuclear Physics A

2008

DOI: 10.1016/j.nuclphysa.2008.07.015

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Spontaneous chiral symmetry breaking in the massless linear sigma model by fermion and boson loop corrections

Setsuo Tamenaga

H. Toki

Akihiro Haga

et al.

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2011

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Cited by 2 publications

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Relativistic chiral mean field model for finite nuclei

Ogawa

Toki

2011

Nuclear Physics A

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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.

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Relativistic chiral mean field model for finite nuclei

Ogawa

Toki

2011

Nuclear Physics A

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Procedure for Generating Equations in Linear Sigma Model

Fariborz

2011

Int. J. Mod. Phys. A

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Spontaneous chiral symmetry breaking in the massless linear sigma model by fermion and boson loop corrections

Cited by 2 publications

References 50 publications

Relativistic chiral mean field model for finite nuclei

Relativistic chiral mean field model for finite nuclei

Procedure for Generating Equations in Linear Sigma Model

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