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Temperature in Fermion Systems and the Chiral Fermion Determinant
We give an interpretation to the issue of the chiral determinant in the heat-kernel approach. The extra dimension (5-th dimension) is interpreted as temperature. The 1+4 dim Dirac equation is naturally derived by the Wick rotation for the temperature. In order to define a ``good'' temperat...
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Lenguaje: | eng |
Publicado: |
2000
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Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.61.055001 http://cds.cern.ch/record/370754 |
_version_ | 1780893100884885504 |
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author | Ichinose, S |
author_facet | Ichinose, S |
author_sort | Ichinose, S |
collection | CERN |
description | We give an interpretation to the issue of the chiral determinant in the heat-kernel approach. The extra dimension (5-th dimension) is interpreted as temperature. The 1+4 dim Dirac equation is naturally derived by the Wick rotation for the temperature. In order to define a ``good'' temperature, we choose those solutions of the Dirac equation which propagate in a fixed direction in the extra coordinate. This choice fixes the regularization of the fermion determinant. The 1+4 dimensional Dirac mass ($M$) is naturally introduced and the relation: $|$4 dim electron momentum$|$ $\ll$ $|M|$ $\ll$ ultraviolet cut-off, naturally appears. The chiral anomaly is explicitly derived for the 2 dim Abelian model. Consistent and covariant anomalies appear depending on the choice of propagators. |
id | cern-370754 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2000 |
record_format | invenio |
spelling | cern-3707542019-09-30T06:29:59Zdoi:10.1103/PhysRevD.61.055001http://cds.cern.ch/record/370754engIchinose, STemperature in Fermion Systems and the Chiral Fermion DeterminantParticle Physics - TheoryWe give an interpretation to the issue of the chiral determinant in the heat-kernel approach. The extra dimension (5-th dimension) is interpreted as temperature. The 1+4 dim Dirac equation is naturally derived by the Wick rotation for the temperature. In order to define a ``good'' temperature, we choose those solutions of the Dirac equation which propagate in a fixed direction in the extra coordinate. This choice fixes the regularization of the fermion determinant. The 1+4 dimensional Dirac mass ($M$) is naturally introduced and the relation: $|$4 dim electron momentum$|$ $\ll$ $|M|$ $\ll$ ultraviolet cut-off, naturally appears. The chiral anomaly is explicitly derived for the 2 dim Abelian model. Consistent and covariant anomalies appear depending on the choice of propagators.hep-th/9811094oai:cds.cern.ch:3707542000 |
spellingShingle | Particle Physics - Theory Ichinose, S Temperature in Fermion Systems and the Chiral Fermion Determinant |
title | Temperature in Fermion Systems and the Chiral Fermion Determinant |
title_full | Temperature in Fermion Systems and the Chiral Fermion Determinant |
title_fullStr | Temperature in Fermion Systems and the Chiral Fermion Determinant |
title_full_unstemmed | Temperature in Fermion Systems and the Chiral Fermion Determinant |
title_short | Temperature in Fermion Systems and the Chiral Fermion Determinant |
title_sort | temperature in fermion systems and the chiral fermion determinant |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1103/PhysRevD.61.055001 http://cds.cern.ch/record/370754 |
work_keys_str_mv | AT ichinoses temperatureinfermionsystemsandthechiralfermiondeterminant |