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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...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2015
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP05(2016)037 http://cds.cern.ch/record/2112526 |
_version_ | 1780948927841828864 |
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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. |
id | cern-2112526 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2015 |
record_format | invenio |
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 |