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Precision Test of Quark Mass Textures: A Model Independent Approach

Using a Monte Carlo method, we have directly extracted from the available measurements, the hierarchies among the different elements of the quark mass matrices. To do that, we have first introduced a model independent parameterization for two generic class of models: those based on Abelian symmetrie...

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Detalles Bibliográficos
Autores principales: Caravaglios, F., Roudeau, P., Stocchi, A.
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(02)00255-9
http://cds.cern.ch/record/537451
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author Caravaglios, F.
Roudeau, P.
Stocchi, A.
author_facet Caravaglios, F.
Roudeau, P.
Stocchi, A.
author_sort Caravaglios, F.
collection CERN
description Using a Monte Carlo method, we have directly extracted from the available measurements, the hierarchies among the different elements of the quark mass matrices. To do that, we have first introduced a model independent parameterization for two generic class of models: those based on Abelian symmetries and those inspired by a U(2) horizontal symmetry. So, matrix entries are proportional to some epsilon^t, with epsilon1 and the t's are different free exponents that we determine from the data through a statistically well defined procedure. We have found that the experimental data poorly constrain the Abelian scenarios. Instead, in non Abelian scenarios, these t-exponents are strongly constrained by the present data. We have found that contrary to a naive U(2) horizontal symmetry expectation, quark mass matrices turn out to be not symmetric. Two solutions emerge: one with M_{32}^{{down}} M_{23}^{down}} and M_{21}^{up}>> M_{12}^{{up}}; and a second one with slight asymmetries only in the light quark sector, namely M_{21}^{up} < M_{12}^{up} and M_{21}^{down}>M_{12}^{down}.
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spelling cern-5374512019-09-30T06:29:59Zdoi:10.1016/S0550-3213(02)00255-9http://cds.cern.ch/record/537451engCaravaglios, F.Roudeau, P.Stocchi, A.Precision Test of Quark Mass Textures: A Model Independent ApproachParticle Physics - PhenomenologyUsing a Monte Carlo method, we have directly extracted from the available measurements, the hierarchies among the different elements of the quark mass matrices. To do that, we have first introduced a model independent parameterization for two generic class of models: those based on Abelian symmetries and those inspired by a U(2) horizontal symmetry. So, matrix entries are proportional to some epsilon^t, with epsilon1 and the t's are different free exponents that we determine from the data through a statistically well defined procedure. We have found that the experimental data poorly constrain the Abelian scenarios. Instead, in non Abelian scenarios, these t-exponents are strongly constrained by the present data. We have found that contrary to a naive U(2) horizontal symmetry expectation, quark mass matrices turn out to be not symmetric. Two solutions emerge: one with M_{32}^{{down}} M_{23}^{down}} and M_{21}^{up}>> M_{12}^{{up}}; and a second one with slight asymmetries only in the light quark sector, namely M_{21}^{up} < M_{12}^{up} and M_{21}^{down}>M_{12}^{down}.Using a Monte Carlo method, we have directly extracted from the available measurements, the hierarchies among the different elements of the quark mass matrices. To do that, we have first introduced a model independent parameterization for two generic class of models: those based on Abelian symmetries and those inspired by a U(2) horizontal symmetry. So, matrix entries are proportional to some epsilon^t, with epsilon<<1 and the t's are different free exponents that we determine from the data through a statistically well defined procedure. We have found that the experimental data poorly constrain the Abelian scenarios. Instead, in non Abelian scenarios, these t-exponents are strongly constrained by the present data. We have found that contrary to a naive U(2) horizontal symmetry expectation, quark mass matrices turn out to be not symmetric. Two solutions emerge: one with M_{32}^{{down}}>> M_{23}^{down}} and M_{21}^{up}>> M_{12}^{{up}}: and a second one with slight asymmetries only in the light quark sector, namely M_{21}^{up} < M_{12}^{up} and M_{21}^{down}>M_{12}^{down}.Using a Monte Carlo method, we have directly extracted from the available measurements, the hierarchies among the different elements of the quark mass matrices. To do that, we have first introduced a model independent parameterization for two generic class of models: those based on Abelian symmetries and those inspired by a U(2) horizontal symmetry. So, matrix entries are proportional to some epsilon^t, with epsilon<<1 and the t's are different free exponents that we determine from the data through a statistically well defined procedure. We have found that the experimental data poorly constrain the Abelian scenarios. Instead, in non Abelian scenarios, these t-exponents are strongly constrained by the present data. We have found that contrary to a naive U(2) horizontal symmetry expectation, quark mass matrices turn out to be not symmetric. Two solutions emerge: one with M_{32}^{{down}}>> M_{23}^{down}} and M_{21}^{up}>> M_{12}^{{up}}: and a second one with slight asymmetries only in the light quark sector, namely M_{21}^{up} < M_{12}^{up} and M_{21}^{down}>M_{12}^{down}.Using a Monte Carlo method, we have directly extracted from the available measurements, the hierarchies among the different elements of the quark mass matrices. To do that, we have first introduced a model independent parameterization for two generic class of models: those based on Abelian symmetries and those inspired by a U(2) horizontal symmetry. So, matrix entries are proportional to some epsilon^t, with epsilon<<1 and the t's are different free exponents that we determine from the data through a statistically well defined procedure. We have found that the experimental data poorly constrain the Abelian scenarios. Instead, in non Abelian scenarios, these t-exponents are strongly constrained by the present data. We have found that contrary to a naive U(2) horizontal symmetry expectation, quark mass matrices turn out to be not symmetric. Two solutions emerge: one with M_{32}^{{down}}>> M_{23}^{down}} and M_{21}^{up}>> M_{12}^{{up}}: and a second one with slight asymmetries only in the light quark sector, namely M_{21}^{up} < M_{12}^{up} and M_{21}^{down}>M_{12}^{down}.Using a Monte Carlo method, we have directly extracted from the available measurements, the hierarchies among the different elements of the quark mass matrices. To do that, we have first introduced a model-independent parameterization for two generic class of models: those based on Abelian symmetries and those inspired by a U (2) horizontal symmetry. So, matrix entries are proportional to some ϵ t , with ϵ ⪡1 and the t 's are different free exponents that we determine from the data through a statistically well defined procedure. We have found that the experimental data poorly constrain the Abelian scenarios.hep-ph/0202055IFUM-702-FTIFUM-702-FTLAL-2002-94oai:cds.cern.ch:5374512002-02-06
spellingShingle Particle Physics - Phenomenology
Caravaglios, F.
Roudeau, P.
Stocchi, A.
Precision Test of Quark Mass Textures: A Model Independent Approach
title Precision Test of Quark Mass Textures: A Model Independent Approach
title_full Precision Test of Quark Mass Textures: A Model Independent Approach
title_fullStr Precision Test of Quark Mass Textures: A Model Independent Approach
title_full_unstemmed Precision Test of Quark Mass Textures: A Model Independent Approach
title_short Precision Test of Quark Mass Textures: A Model Independent Approach
title_sort precision test of quark mass textures: a model independent approach
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(02)00255-9
http://cds.cern.ch/record/537451
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