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Flavour from the Planck scale to the electroweak scale
We discuss a theory of flavour in which Higgs Yukawa couplings are related to those of the new scalar triplet leptoquark and/or $Z'$ responsible for $R_{K^{(*)}}$, with all couplings arising effectively from mixing with a vector-like fourth family, whose mass may be anywhere from the Planck sca...
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Lenguaje: | eng |
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2019
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Acceso en línea: | http://cds.cern.ch/record/2758993 |
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author | King, S.F. |
author_facet | King, S.F. |
author_sort | King, S.F. |
collection | CERN |
description | We discuss a theory of flavour in which Higgs Yukawa couplings are related to those of the new scalar triplet leptoquark and/or $Z'$ responsible for $R_{K^{(*)}}$, with all couplings arising effectively from mixing with a vector-like fourth family, whose mass may be anywhere from the Planck scale to the electroweak scale for the leptoquarks explanation, but is pinned down to the TeV scale if the $Z'$ exchange plays a role. However, in this particular model, only leptoquark exchange can contribute significantly to $R_{K^{(*)}}$, since $Z'$ exchange is too constrained from $B_s$ mixing and $\tau \rightarrow 3 \mu$, although other Higgs Yukawa matrix structures may allow it. |
id | cern-2758993 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
record_format | invenio |
spelling | cern-27589932023-02-16T08:51:03Zhttp://cds.cern.ch/record/2758993engKing, S.F.Flavour from the Planck scale to the electroweak scalehep-phParticle Physics - PhenomenologyWe discuss a theory of flavour in which Higgs Yukawa couplings are related to those of the new scalar triplet leptoquark and/or $Z'$ responsible for $R_{K^{(*)}}$, with all couplings arising effectively from mixing with a vector-like fourth family, whose mass may be anywhere from the Planck scale to the electroweak scale for the leptoquarks explanation, but is pinned down to the TeV scale if the $Z'$ exchange plays a role. However, in this particular model, only leptoquark exchange can contribute significantly to $R_{K^{(*)}}$, since $Z'$ exchange is too constrained from $B_s$ mixing and $\tau \rightarrow 3 \mu$, although other Higgs Yukawa matrix structures may allow it.arXiv:1905.02660oai:cds.cern.ch:27589932019 |
spellingShingle | hep-ph Particle Physics - Phenomenology King, S.F. Flavour from the Planck scale to the electroweak scale |
title | Flavour from the Planck scale to the electroweak scale |
title_full | Flavour from the Planck scale to the electroweak scale |
title_fullStr | Flavour from the Planck scale to the electroweak scale |
title_full_unstemmed | Flavour from the Planck scale to the electroweak scale |
title_short | Flavour from the Planck scale to the electroweak scale |
title_sort | flavour from the planck scale to the electroweak scale |
topic | hep-ph Particle Physics - Phenomenology |
url | http://cds.cern.ch/record/2758993 |
work_keys_str_mv | AT kingsf flavourfromtheplanckscaletotheelectroweakscale |