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Resolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ Decays

It is well known that $\sin(2\beta)$, where $\beta$ is one of the angles of the unitarity triangle of the CKM matrix, can be determined in a theoretically clean way by measuring mixing-induced CP violation in the decay $B_d \to J/\psi K_S$. Another clean extraction of this CKM angle is provided by t...

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Detalles Bibliográficos
Autores principales: Dighe, Amol S., Dunietz, Isard, Fleischer, Robert
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(98)00680-7
http://cds.cern.ch/record/351749
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author Dighe, Amol S.
Dunietz, Isard
Fleischer, Robert
author_facet Dighe, Amol S.
Dunietz, Isard
Fleischer, Robert
author_sort Dighe, Amol S.
collection CERN
description It is well known that $\sin(2\beta)$, where $\beta$ is one of the angles of the unitarity triangle of the CKM matrix, can be determined in a theoretically clean way by measuring mixing-induced CP violation in the decay $B_d \to J/\psi K_S$. Another clean extraction of this CKM angle is provided by the time-dependent angular distribution for the decay products of $B_d \to J/\psi(\to l^+l^-) K^{\ast0}(\to \pi^0 K_S)$, where we have more observables at our disposal than in the case of $B_d \to J/\psi K_S$, so that in addition to a sign ambiguity remains in $\cos(2\beta)$. If it could be resolved, a discrete ambiguity in the extraction of the CKM angle $\beta$ could be resolved as well, which would allow a more incisive test of the CKM model of CP violation. This note shows that detailed time-dependent studies of $B_{u,d} \to J/\psi K^{\ast}$ and $B_s \to J/\psi \phi$ decay processes can determine the sign of of the CKM angle $\beta$.
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publishDate 1998
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spelling cern-3517492023-01-31T09:36:58Zdoi:10.1016/S0370-2693(98)00680-7http://cds.cern.ch/record/351749engDighe, Amol S.Dunietz, IsardFleischer, RobertResolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ DecaysParticle Physics - PhenomenologyIt is well known that $\sin(2\beta)$, where $\beta$ is one of the angles of the unitarity triangle of the CKM matrix, can be determined in a theoretically clean way by measuring mixing-induced CP violation in the decay $B_d \to J/\psi K_S$. Another clean extraction of this CKM angle is provided by the time-dependent angular distribution for the decay products of $B_d \to J/\psi(\to l^+l^-) K^{\ast0}(\to \pi^0 K_S)$, where we have more observables at our disposal than in the case of $B_d \to J/\psi K_S$, so that in addition to a sign ambiguity remains in $\cos(2\beta)$. If it could be resolved, a discrete ambiguity in the extraction of the CKM angle $\beta$ could be resolved as well, which would allow a more incisive test of the CKM model of CP violation. This note shows that detailed time-dependent studies of $B_{u,d} \to J/\psi K^{\ast}$ and $B_s \to J/\psi \phi$ decay processes can determine the sign of of the CKM angle $\beta$.It is well known that $\sin(2\beta)$, where $\beta$ is one of the angles of the unitarity triangle of the CKM matrix, can be determined in a theoretically clean way by measuring mixing-induced CP violation in the decay $B_d \to J/\psi K_S$. Another clean extraction of this CKM angle is provided by the time-dependent angular distribution for the decay products of $B_d \to J/\psi(\to l^+l^-) K^{\ast0}(\to \pi^0 K_S)$, where we have more observables at our disposal than in the case of $B_d \to J/\psi K_S$, so that in addition to $\sin(2\beta)$ also $\cos(2\beta)$ can be probed in a direct way. Unfortunately a sign ambiguity remains in $\cos(2\beta)$. If it could be resolved, a discrete ambiguity in the extraction of the CKM angle $\beta$ could be resolved as well, which would allow a more incisive test of the CKM model of CP violation. This note shows that detailed time-dependent studies of $B_{u,d} \to J/\psi K^{\ast}$ and $B_s \to J/\psi \phi$ decay processes can determine the sign of $\cos(2\beta)$, thereby removing the corresponding ambiguity in the extraction of the CKM angle $\beta$.hep-ph/9804254CERN-TH-98-123FERMILAB-PUB-98-101-TIC-98-35CERN-TH-98-123FERMILAB-PUB-98-101-TIC-98-34oai:cds.cern.ch:3517491998-04-09
spellingShingle Particle Physics - Phenomenology
Dighe, Amol S.
Dunietz, Isard
Fleischer, Robert
Resolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ Decays
title Resolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ Decays
title_full Resolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ Decays
title_fullStr Resolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ Decays
title_full_unstemmed Resolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ Decays
title_short Resolving a Discrete Ambiguity in the CKM Angle $\beta$ through $B_{u,d} \rightarrow J/\psi K^*$ and $B_s \rightarrow J/\psi \phi$ Decays
title_sort resolving a discrete ambiguity in the ckm angle $\beta$ through $b_{u,d} \rightarrow j/\psi k^*$ and $b_s \rightarrow j/\psi \phi$ decays
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(98)00680-7
http://cds.cern.ch/record/351749
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AT fleischerrobert resolvingadiscreteambiguityintheckmanglebetathroughbudrightarrowjpsikandbsrightarrowjpsiphidecays