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The Algebraic Method

Combining the effect of an intermediate renormalization prescription (zero momentum subtraction) and the background field method (BFM), we show that the algebraic renormalization procedure needed for the computation of radiative corrections within non-invariant regularization schemes is drastically...

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Detalles Bibliográficos
Autores principales: Grassi, P.A., Hurth, T., Steinhauser, M.
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(01)00303-0
http://cds.cern.ch/record/485700
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author Grassi, P.A.
Hurth, T.
Steinhauser, M.
author_facet Grassi, P.A.
Hurth, T.
Steinhauser, M.
author_sort Grassi, P.A.
collection CERN
description Combining the effect of an intermediate renormalization prescription (zero momentum subtraction) and the background field method (BFM), we show that the algebraic renormalization procedure needed for the computation of radiative corrections within non-invariant regularization schemes is drastically simplified. The present technique is suitable for gauge models and, here, is applied to the Standard Model. The use of the BFM allows a powerful organization of the counterterms and avoids complicated Slavnov-Taylor identities. Furthermore, the Becchi-Rouet-Stora-Tyutin (BRST) variation of background fields plays a special role in disentangling Ward-Takahashi identities (WTI) and Slavnov-Taylor identities (STI). Finally, the strategy to be applied to physical processes is exemplified for the process $b\to s\gamma$.
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spelling cern-4857002023-10-04T05:57:28Zdoi:10.1016/S0550-3213(01)00303-0http://cds.cern.ch/record/485700engGrassi, P.A.Hurth, T.Steinhauser, M.The Algebraic MethodParticle Physics - PhenomenologyCombining the effect of an intermediate renormalization prescription (zero momentum subtraction) and the background field method (BFM), we show that the algebraic renormalization procedure needed for the computation of radiative corrections within non-invariant regularization schemes is drastically simplified. The present technique is suitable for gauge models and, here, is applied to the Standard Model. The use of the BFM allows a powerful organization of the counterterms and avoids complicated Slavnov-Taylor identities. Furthermore, the Becchi-Rouet-Stora-Tyutin (BRST) variation of background fields plays a special role in disentangling Ward-Takahashi identities (WTI) and Slavnov-Taylor identities (STI). Finally, the strategy to be applied to physical processes is exemplified for the process $b\to s\gamma$.Combining the effect of an intermediate renormalization prescription (zero momentum subtraction) and the background field method (BFM), we show that the algebraic renormalization procedure needed for the computation of radiative corrections within non-invariant regularization schemes is drastically simplified. The present technique is suitable for gauge models and, here, is applied to the Standard Model. The use of the BFM allows a powerful organization of the counterterms and avoids complicated Slavnov-Taylor identities. Furthermore, the Becchi-Rouet-Stora-Tyutin (BRST) variation of background fields plays a special role in disentangling Ward-Takahashi identities (WTI) and Slavnov-Taylor identities (STI). Finally, the strategy to be applied to physical processes is exemplified for the process $b\to s\gamma$.Combining the effect of an intermediate renormalization prescription (zero momentum subtraction) and the background field method (BFM), we show that the algebraic renormalization procedure needed for the computation of radiative corrections within non-invariant regularization schemes is drastically simplified. The present technique is suitable for gauge models and, here, is applied to the Standard Model. The use of the BFM allows a powerful organization of the counterterms and avoids complicated Slavnov–Taylor identities. Furthermore, the Becchi–Rouet–Stora–Tyutin (BRST) variation of background fields plays a special role in disentangling Ward–Takahashi identities (WTI) and Slavnov–Taylor identities (STI). Finally, the strategy to be applied to physical processes is exemplified for the process b → sγ .hep-ph/0102005NYU-TH-00-09-09CERN-TH-2001-002DESY-01-008CERN-TH-2001-002DESY-2001-008NYU-TH-2000-09-09DESY-01-008oai:cds.cern.ch:4857002001-02-01
spellingShingle Particle Physics - Phenomenology
Grassi, P.A.
Hurth, T.
Steinhauser, M.
The Algebraic Method
title The Algebraic Method
title_full The Algebraic Method
title_fullStr The Algebraic Method
title_full_unstemmed The Algebraic Method
title_short The Algebraic Method
title_sort algebraic method
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(01)00303-0
http://cds.cern.ch/record/485700
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