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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...

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Detalles Bibliográficos
Autores principales: Colladay, Don, McDonald, Patrick, Potting, Robertus
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.89.085014
http://cds.cern.ch/record/1641101
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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
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AT mcdonaldpatrick guptableulerphotonquantizationinthesme
AT pottingrobertus guptableulerphotonquantizationinthesme