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Matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions

New physics realized above the electroweak scale can be encoded in a model independent way in the Wilson coefficients of higher dimensional operators which are invariant under the Standard Model gauge group. In this article, we study the matching of the $SU(3)_C \times SU(2)_L \times U(1)_Y$ gauge i...

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Autores principales: Aebischer, Jason, Crivellin, Andreas, Fael, Matteo, Greub, Christoph
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP05(2016)037
http://cds.cern.ch/record/2112526
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author Aebischer, Jason
Crivellin, Andreas
Fael, Matteo
Greub, Christoph
author_facet Aebischer, Jason
Crivellin, Andreas
Fael, Matteo
Greub, Christoph
author_sort Aebischer, Jason
collection CERN
description New physics realized above the electroweak scale can be encoded in a model independent way in the Wilson coefficients of higher dimensional operators which are invariant under the Standard Model gauge group. In this article, we study the matching of the $SU(3)_C \times SU(2)_L \times U(1)_Y$ gauge invariant dim-6 operators on the standard $B$ physics Hamiltonian relevant for $b \to s$ and $b\to c$ transitions. The matching is performed at the electroweak scale (after spontaneous symmetry breaking) by integrating out the top quark, $W$, $Z$ and the Higgs particle. We first carry out the matching of the dim-6 operators that give a contribution at tree level to the low energy Hamiltonian. In a second step, we identify those gauge invariant operators that do not enter $b \to s$ transitions already at tree level, but can give relevant one-loop matching effects.
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institution Organización Europea para la Investigación Nuclear
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publishDate 2015
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spelling cern-21125262022-08-10T12:43:28Zdoi:10.1007/JHEP05(2016)037http://cds.cern.ch/record/2112526engAebischer, JasonCrivellin, AndreasFael, MatteoGreub, ChristophMatching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitionsParticle Physics - PhenomenologyNew physics realized above the electroweak scale can be encoded in a model independent way in the Wilson coefficients of higher dimensional operators which are invariant under the Standard Model gauge group. In this article, we study the matching of the $SU(3)_C \times SU(2)_L \times U(1)_Y$ gauge invariant dim-6 operators on the standard $B$ physics Hamiltonian relevant for $b \to s$ and $b\to c$ transitions. The matching is performed at the electroweak scale (after spontaneous symmetry breaking) by integrating out the top quark, $W$, $Z$ and the Higgs particle. We first carry out the matching of the dim-6 operators that give a contribution at tree level to the low energy Hamiltonian. In a second step, we identify those gauge invariant operators that do not enter $b \to s$ transitions already at tree level, but can give relevant one-loop matching effects.New physics realized above the electroweak scale can be encoded in a model independent way in the Wilson coefficients of higher dimensional operators which are in-variant under the Standard Model gauge group. In this article, we study the matching of the SU(3)$_{C}$ × SU(2)$_{L}$ × U(1)$_{Y}$ gauge invariant dimension-six operators on the standard B physics Hamiltonian relevant for b → s and b → c transitions. The matching is performed at the electroweak scale (after spontaneous symmetry breaking) by integrating out the top quark, W , Z and the Higgs particle. We first carry out the matching of the dimension-six operators that give a contribution at tree level to the low energy Hamiltonian. In a second step, we identify those gauge invariant operators that do not enter b → s transitions already at tree level, but can give relevant one-loop matching effects.New physics realized above the electroweak scale can be encoded in a model independent way in the Wilson coefficients of higher dimensional operators which are invariant under the Standard Model gauge group. In this article, we study the matching of the $SU(3)_C \times SU(2)_L \times U(1)_Y$ gauge invariant dim-6 operators on the standard $B$ physics Hamiltonian relevant for $b \to s$ and $b\to c$ transitions. The matching is performed at the electroweak scale (after spontaneous symmetry breaking) by integrating out the top quark, $W$, $Z$ and the Higgs particle. We first carry out the matching of the dim-6 operators that give a contribution at tree level to the low energy Hamiltonian. In a second step, we identify those gauge invariant operators that do not enter $b \to s$ transitions already at tree level, but can give relevant one-loop matching effects.arXiv:1512.02830CERN-PH-TH-2015-278CERN-PH-TH-2015-278oai:cds.cern.ch:21125262015-12-09
spellingShingle Particle Physics - Phenomenology
Aebischer, Jason
Crivellin, Andreas
Fael, Matteo
Greub, Christoph
Matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions
title Matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions
title_full Matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions
title_fullStr Matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions
title_full_unstemmed Matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions
title_short Matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions
title_sort matching of gauge invariant dimension-six operators for $b\to s$ and $b\to c$ transitions
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP05(2016)037
http://cds.cern.ch/record/2112526
work_keys_str_mv AT aebischerjason matchingofgaugeinvariantdimensionsixoperatorsforbtosandbtoctransitions
AT crivellinandreas matchingofgaugeinvariantdimensionsixoperatorsforbtosandbtoctransitions
AT faelmatteo matchingofgaugeinvariantdimensionsixoperatorsforbtosandbtoctransitions
AT greubchristoph matchingofgaugeinvariantdimensionsixoperatorsforbtosandbtoctransitions