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Effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplings

LHCb reported anomalies in $B\to K^* \mu^+\mu^-$, $B_s\to\phi\mu^+\mu^-$ and $R(K)=B\to K \mu^+\mu^-/B\to K e^+e^-$. Furthermore, BaBar, BELLE and LHCb found hints for the violation of lepton flavour universality violation in $R(D^{(*)})=B\to D^{(*)}\tau\nu/B\to D^{(*)}\ell\nu$. In this note we reex...

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Detalles Bibliográficos
Autores principales: Calibbi, Lorenzo, Crivellin, Andreas, Ota, Toshihiko
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevLett.115.181801
http://cds.cern.ch/record/2024070
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author Calibbi, Lorenzo
Crivellin, Andreas
Ota, Toshihiko
author_facet Calibbi, Lorenzo
Crivellin, Andreas
Ota, Toshihiko
author_sort Calibbi, Lorenzo
collection CERN
description LHCb reported anomalies in $B\to K^* \mu^+\mu^-$, $B_s\to\phi\mu^+\mu^-$ and $R(K)=B\to K \mu^+\mu^-/B\to K e^+e^-$. Furthermore, BaBar, BELLE and LHCb found hints for the violation of lepton flavour universality violation in $R(D^{(*)})=B\to D^{(*)}\tau\nu/B\to D^{(*)}\ell\nu$. In this note we reexamine these decays and their correlations to $B\to K^{(*)}\nu\bar{\nu}$ using gauge invariant dim-6 operators. For the numerical analysis we focus on scenarios in which new physics couples, in the interaction eigenbasis, to third generation quarks and lepton only. We conclude that such a setup can explain the $b\to s\mu^+\mu^-$ data simultaneously with $R(D^{(*)})$ for small mixing angles in the lepton sector (of the order of $\pi/16$) and very small mixing angles in the quark sector (smaller than $V_{cb}$). In these region of parameter space $B\to K^{(*)}\tau\mu$ and $B_s\to \tau\mu$ can be order $10^{-6}$. Possible UV completions are briefly discussed.
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institution Organización Europea para la Investigación Nuclear
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publishDate 2015
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spelling cern-20240702022-08-10T12:54:14Zdoi:10.1103/PhysRevLett.115.181801http://cds.cern.ch/record/2024070engCalibbi, LorenzoCrivellin, AndreasOta, ToshihikoEffective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplingsParticle Physics - PhenomenologyLHCb reported anomalies in $B\to K^* \mu^+\mu^-$, $B_s\to\phi\mu^+\mu^-$ and $R(K)=B\to K \mu^+\mu^-/B\to K e^+e^-$. Furthermore, BaBar, BELLE and LHCb found hints for the violation of lepton flavour universality violation in $R(D^{(*)})=B\to D^{(*)}\tau\nu/B\to D^{(*)}\ell\nu$. In this note we reexamine these decays and their correlations to $B\to K^{(*)}\nu\bar{\nu}$ using gauge invariant dim-6 operators. For the numerical analysis we focus on scenarios in which new physics couples, in the interaction eigenbasis, to third generation quarks and lepton only. We conclude that such a setup can explain the $b\to s\mu^+\mu^-$ data simultaneously with $R(D^{(*)})$ for small mixing angles in the lepton sector (of the order of $\pi/16$) and very small mixing angles in the quark sector (smaller than $V_{cb}$). In these region of parameter space $B\to K^{(*)}\tau\mu$ and $B_s\to \tau\mu$ can be order $10^{-6}$. Possible UV completions are briefly discussed.The LHCb Collaboration reported anomalies in B→K*μ+μ-, Bs→ϕμ+μ-, and R(K)=B→Kμ+μ-/B→Ke+e-. Furthermore, BABAR, BELLE, and LHCb Collaborations found hints for the violation of lepton-flavor universality violation in R(D(*))=B→D(*)τν/B→D(*)ℓν. In this Letter we reexamine these decays and their correlations to B→K(*)νν¯ using gauge invariant dim-6 operators. For the numerical analysis we focus on scenarios in which new physics couples, in the interaction eigenbasis, to third generation quarks and lepton only. We conclude that such a setup can explain the b→sμ+μ- data simultaneously with R(D(*)) for small mixing angles in the lepton sector (of the order of π/16) and very small mixing angles in the quark sector (smaller than Vcb). In these regions of parameter space, B→K(*)τμ and Bs→τμ can be order 10-6. Possible UV completions are briefly discussed.LHCb reported anomalies in $B\to K^* \mu^+\mu^-$, $B_s\to\phi\mu^+\mu^-$ and $R(K)=B\to K \mu^+\mu^-/B\to K e^+e^-$. Furthermore, BaBar, BELLE and LHCb found hints for the violation of lepton flavour universality violation in $R(D^{(*)})=B\to D^{(*)}\tau\nu/B\to D^{(*)}\ell\nu$. In this note we reexamine these decays and their correlations to $B\to K^{(*)}\nu\bar{\nu}$ using gauge invariant dim-6 operators. For the numerical analysis we focus on scenarios in which new physics couples, in the interaction eigenbasis, to third generation quarks and lepton only. We conclude that such a setup can explain the $b\to s\mu^+\mu^-$ data simultaneously with $R(D^{(*)})$ for small mixing angles in the lepton sector (of the order of $\pi/16$) and very small mixing angles in the quark sector (smaller than $V_{cb}$). In these region of parameter space $B\to K^{(*)}\tau\mu$ and $B_s\to \tau\mu$ can be order $10^{-6}$. Possible UV completions are briefly discussed.arXiv:1506.02661CERN-PH-TH-2015-134STUPP-15-222CERN-PH-TH-2015-134STUPP-15-222oai:cds.cern.ch:20240702015-06-08
spellingShingle Particle Physics - Phenomenology
Calibbi, Lorenzo
Crivellin, Andreas
Ota, Toshihiko
Effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplings
title Effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplings
title_full Effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplings
title_fullStr Effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplings
title_full_unstemmed Effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplings
title_short Effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $B\to K^{(*)}\nu\bar{\nu}$ and $B\to D^{(*)}\tau\nu$ with third generation couplings
title_sort effective field theory approach to $b\to s\ell\ell^{(\prime)}$, $b\to k^{(*)}\nu\bar{\nu}$ and $b\to d^{(*)}\tau\nu$ with third generation couplings
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevLett.115.181801
http://cds.cern.ch/record/2024070
work_keys_str_mv AT calibbilorenzo effectivefieldtheoryapproachtobtosellellprimebtoknubarnuandbtodtaunuwiththirdgenerationcouplings
AT crivellinandreas effectivefieldtheoryapproachtobtosellellprimebtoknubarnuandbtodtaunuwiththirdgenerationcouplings
AT otatoshihiko effectivefieldtheoryapproachtobtosellellprimebtoknubarnuandbtodtaunuwiththirdgenerationcouplings