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Analysis of General Power Counting Rules in Effective Field Theory

We derive the general counting rules for a quantum effective field theory (EFT) in $\mathsf{d}$ dimensions. The rules are valid for strongly and weakly coupled theories, and predict that all kinetic energy terms are canonically normalized. They determine the energy dependence of scattering cross sec...

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Autores principales: Gavela, B.M., Jenkins, E.E., Manohar, A.V., Merlo, L.
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1140/epjc/s10052-016-4332-1
http://cds.cern.ch/record/2127661
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author Gavela, B.M.
Jenkins, E.E.
Manohar, A.V.
Merlo, L.
author_facet Gavela, B.M.
Jenkins, E.E.
Manohar, A.V.
Merlo, L.
author_sort Gavela, B.M.
collection CERN
description We derive the general counting rules for a quantum effective field theory (EFT) in $\mathsf{d}$ dimensions. The rules are valid for strongly and weakly coupled theories, and predict that all kinetic energy terms are canonically normalized. They determine the energy dependence of scattering cross sections in the range of validity of the EFT expansion. The size of cross sections is controlled by the $\Lambda$ power counting of EFT, not by chiral counting, even for chiral perturbation theory ($\chi$PT). The relation between $\Lambda$ and $f$ is generalized to $\mathsf{d}$ dimensions. We show that the naive dimensional analysis $4\pi$ counting is related to $\hbar$ counting. The EFT counting rules are applied to $\chi$PT, to Standard Model EFT and to the non-trivial case of Higgs EFT, which combines the $\Lambda$ and chiral counting rules within a single theory.
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-21276612022-08-10T12:48:39Zdoi:10.1140/epjc/s10052-016-4332-1http://cds.cern.ch/record/2127661engGavela, B.M.Jenkins, E.E.Manohar, A.V.Merlo, L.Analysis of General Power Counting Rules in Effective Field TheoryParticle Physics - PhenomenologyWe derive the general counting rules for a quantum effective field theory (EFT) in $\mathsf{d}$ dimensions. The rules are valid for strongly and weakly coupled theories, and predict that all kinetic energy terms are canonically normalized. They determine the energy dependence of scattering cross sections in the range of validity of the EFT expansion. The size of cross sections is controlled by the $\Lambda$ power counting of EFT, not by chiral counting, even for chiral perturbation theory ($\chi$PT). The relation between $\Lambda$ and $f$ is generalized to $\mathsf{d}$ dimensions. We show that the naive dimensional analysis $4\pi$ counting is related to $\hbar$ counting. The EFT counting rules are applied to $\chi$PT, to Standard Model EFT and to the non-trivial case of Higgs EFT, which combines the $\Lambda$ and chiral counting rules within a single theory.We derive the general counting rules for a quantum effective field theory (EFT) in $\mathsf {d}$ dimensions. The rules are valid for strongly and weakly coupled theories, and they predict that all kinetic energy terms are canonically normalized. They determine the energy dependence of scattering cross sections in the range of validity of the EFT expansion. We show that the size of the cross sections is controlled by the $\Lambda $ power counting of EFT, not by chiral counting, even for chiral perturbation theory ( $\chi $ PT). The relation between $\Lambda $ and f is generalized to $\mathsf {d}$ dimensions. We show that the naive dimensional analysis $4\pi $ counting is related to $\hbar $ counting. The EFT counting rules are applied to $\chi $ PT, low-energy weak interactions, Standard Model EFT and the non-trivial case of Higgs EFT.We derive the general counting rules for a quantum effective field theory (EFT) in $\mathsf{d}$ dimensions. The rules are valid for strongly and weakly coupled theories, and predict that all kinetic energy terms are canonically normalized. They determine the energy dependence of scattering cross sections in the range of validity of the EFT expansion. We show that the size of cross sections is controlled by the $\Lambda$ power counting of EFT, not by chiral counting, even for chiral perturbation theory ($\chi$PT). The relation between $\Lambda$ and $f$ is generalized to $\mathsf{d}$ dimensions. We show that the naive dimensional analysis $4\pi$ counting is related to $\hbar$ counting. The EFT counting rules are applied to $\chi$PT, low-energy weak interactions, Standard Model EFT and the non-trivial case of Higgs EFT.arXiv:1601.07551CERN-TH-2016-015FTUAM-16-2IFT-UAM-CSIC-16-006CERN-TH-2016-015FTUAM-16-2IFT-UAM-CSIC-16-006oai:cds.cern.ch:21276612016-01-27
spellingShingle Particle Physics - Phenomenology
Gavela, B.M.
Jenkins, E.E.
Manohar, A.V.
Merlo, L.
Analysis of General Power Counting Rules in Effective Field Theory
title Analysis of General Power Counting Rules in Effective Field Theory
title_full Analysis of General Power Counting Rules in Effective Field Theory
title_fullStr Analysis of General Power Counting Rules in Effective Field Theory
title_full_unstemmed Analysis of General Power Counting Rules in Effective Field Theory
title_short Analysis of General Power Counting Rules in Effective Field Theory
title_sort analysis of general power counting rules in effective field theory
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1140/epjc/s10052-016-4332-1
http://cds.cern.ch/record/2127661
work_keys_str_mv AT gavelabm analysisofgeneralpowercountingrulesineffectivefieldtheory
AT jenkinsee analysisofgeneralpowercountingrulesineffectivefieldtheory
AT manoharav analysisofgeneralpowercountingrulesineffectivefieldtheory
AT merlol analysisofgeneralpowercountingrulesineffectivefieldtheory