
TL;DR
This paper reviews the role of chiral symmetry in QCD, its spontaneous breaking, restoration in hot/dense matter, and related models and experiments exploring these phenomena.
Contribution
It provides a comprehensive overview of chiral symmetry, its breaking, models describing it, and experimental efforts to observe its restoration in nuclear matter.
Findings
Chiral symmetry is approximately realized in light quark QCD.
Models like Nambu-Jona-Lasinio and linear sigma explain chiral dynamics.
Experiments such as heavy-ion collisions probe chiral restoration.
Abstract
We first note the peculiar property of the pion as the pseudoscalar particle, which play the essential role in realizing the basic properties of the nuclear matter such as the density/energy saturations. Then, we introduce the notion of chirality using the Dirac equation, and show how chiralities are mixed in the massive Dirac field with an emphasis on the similarity with the Bogoliubov-Valatin theory of superconductivity. After noting the approximate chiral symmetry in QCD in the light quark sector, we introduce the notion of the spontaneous symmetry breaking, and the Nambu-Goldstone theorem. A remark is given on the U(1) anomaly and its physical consequences. Several chiral quark models of the Nambu-Jona-Lasinio type are introduced with an emphasis to the relevance to QCD, and discuss some consequences of the models. A three-flavor linear sigma model with the determinant…
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