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Gupta-Bleuler Photon Quantization in the SME
Photon quantization is implemented in the standard model extension (SME) using the Gupta-Bleuler method and BRST concepts. The quantization prescription applies to both the birefringent and non-birefringent CPT-even couplings. A curious incompatibility is found between the presence of the Lorentz-vi...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2014
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.89.085014 http://cds.cern.ch/record/1641101 |
_version_ | 1780934857072836608 |
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author | Colladay, Don McDonald, Patrick Potting, Robertus |
author_facet | Colladay, Don McDonald, Patrick Potting, Robertus |
author_sort | Colladay, Don |
collection | CERN |
description | Photon quantization is implemented in the standard model extension (SME) using the Gupta-Bleuler method and BRST concepts. The quantization prescription applies to both the birefringent and non-birefringent CPT-even couplings. A curious incompatibility is found between the presence of the Lorentz-violating terms and the existence of a nontrivial conjugate momentum $\Pi^0$ yielding problems with covariant quantization procedure. Introduction of a mass regulator term can avoid the vanishing of $\Pi^0$ and allows for the implementation of a covariant quantization procedure. Field-theoretic calculations involving the SME photons can then be performed using the mass regulator, similar to the conventional procedure used in electrodynamics for infrared-divergence regulation. |
id | cern-1641101 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-16411012023-03-14T16:34:02Zdoi:10.1103/PhysRevD.89.085014http://cds.cern.ch/record/1641101engColladay, DonMcDonald, PatrickPotting, RobertusGupta-Bleuler Photon Quantization in the SMEParticle Physics - PhenomenologyPhoton quantization is implemented in the standard model extension (SME) using the Gupta-Bleuler method and BRST concepts. The quantization prescription applies to both the birefringent and non-birefringent CPT-even couplings. A curious incompatibility is found between the presence of the Lorentz-violating terms and the existence of a nontrivial conjugate momentum $\Pi^0$ yielding problems with covariant quantization procedure. Introduction of a mass regulator term can avoid the vanishing of $\Pi^0$ and allows for the implementation of a covariant quantization procedure. Field-theoretic calculations involving the SME photons can then be performed using the mass regulator, similar to the conventional procedure used in electrodynamics for infrared-divergence regulation.<p>Photon quantization is implemented in the standard model extension (SME) using the Gupta-Bleuler method and Becchi-Rouet-Stora-Tyutin concepts. The quantization prescription applies to both the birefringent and nonbirefringent <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>C</mml:mi><mml:mi>P</mml:mi><mml:mi>T</mml:mi></mml:mrow></mml:math></inline-formula>-even couplings. A curious incompatibility is found between the presence of the Lorentz-violating terms and the existence of a nontrivial conjugate momentum <inline-formula><mml:math display="inline"><mml:msup><mml:mi mathvariant="normal">Π</mml:mi><mml:mn>0</mml:mn></mml:msup></mml:math></inline-formula> yielding problems with covariant quantization procedure. An introduction of a mass regulator term can avoid the vanishing of <inline-formula><mml:math display="inline"><mml:msup><mml:mi mathvariant="normal">Π</mml:mi><mml:mn>0</mml:mn></mml:msup></mml:math></inline-formula> and allows for the implementation of a covariant quantization procedure. Field-theoretic calculations involving the SME photons can then be performed using the mass regulator, similar to the conventional procedure used in electrodynamics for infrared-divergence regulation.</p>Photon quantization is implemented in the standard model extension (SME) using the Gupta-Bleuler method and BRST concepts. The quantization prescription applies to both the birefringent and non-birefringent CPT-even couplings. A curious incompatibility is found between the presence of the Lorentz-violating terms and the existence of a nontrivial conjugate momentum $\Pi^0$ yielding problems with covariant quantization procedure. Introduction of a mass regulator term can avoid the vanishing of $\Pi^0$ and allows for the implementation of a covariant quantization procedure. Field-theoretic calculations involving the SME photons can then be performed using the mass regulator, similar to the conventional procedure used in electrodynamics for infrared-divergence regulation.arXiv:1401.1173oai:cds.cern.ch:16411012014-01-06 |
spellingShingle | Particle Physics - Phenomenology Colladay, Don McDonald, Patrick Potting, Robertus Gupta-Bleuler Photon Quantization in the SME |
title | Gupta-Bleuler Photon Quantization in the SME |
title_full | Gupta-Bleuler Photon Quantization in the SME |
title_fullStr | Gupta-Bleuler Photon Quantization in the SME |
title_full_unstemmed | Gupta-Bleuler Photon Quantization in the SME |
title_short | Gupta-Bleuler Photon Quantization in the SME |
title_sort | gupta-bleuler photon quantization in the sme |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1103/PhysRevD.89.085014 http://cds.cern.ch/record/1641101 |
work_keys_str_mv | AT colladaydon guptableulerphotonquantizationinthesme AT mcdonaldpatrick guptableulerphotonquantizationinthesme AT pottingrobertus guptableulerphotonquantizationinthesme |