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A Precise determination of B(K) in quenched QCD

The $B_K$ parameter is computed in quenched lattice QCD with Wilson twisted mass fermions. Two variants of tmQCD are used; in both of them the relevant $\Delta S = 2$ four-fermion operator is renormalised multiplicatively. The renormalisation adopted is non-perturbative, with a Schroedinger function...

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Detalles Bibliográficos
Autores principales: Dimopoulos, P., Heitger, J., Palombi, F., Pena, C., Sint, S., Vladikas, A.
Lenguaje:eng
Publicado: 2005
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2006.04.033
http://cds.cern.ch/record/919484
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author Dimopoulos, P.
Heitger, J.
Palombi, F.
Pena, C.
Sint, S.
Vladikas, A.
author_facet Dimopoulos, P.
Heitger, J.
Palombi, F.
Pena, C.
Sint, S.
Vladikas, A.
author_sort Dimopoulos, P.
collection CERN
description The $B_K$ parameter is computed in quenched lattice QCD with Wilson twisted mass fermions. Two variants of tmQCD are used; in both of them the relevant $\Delta S = 2$ four-fermion operator is renormalised multiplicatively. The renormalisation adopted is non-perturbative, with a Schroedinger functional renormalisation condition. Renormalisation group running is also non-perturbative, up to very high energy scales. In one of the two tmQCD frameworks the computations have been performed at the physical $K$-meson mass, thus eliminating the need of mass extrapolations. Simulations have been performed at several lattice spacings and the continuum limit was reached by combining results from both tmQCD regularisations. Finite volume effects have been partially checked and turned out to be small. Exploratory studies have also been performed with non-degenerate valence flavours. The final result for the RGI bag parameter, with all sources of uncertainty (except quenching) under control, is $\hat B_K =0.789 \pm 0.046$.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2005
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spelling cern-9194842023-04-14T03:10:12Zdoi:10.1016/j.nuclphysb.2006.04.033http://cds.cern.ch/record/919484engDimopoulos, P.Heitger, J.Palombi, F.Pena, C.Sint, S.Vladikas, A.A Precise determination of B(K) in quenched QCDParticle Physics - PhenomenologyThe $B_K$ parameter is computed in quenched lattice QCD with Wilson twisted mass fermions. Two variants of tmQCD are used; in both of them the relevant $\Delta S = 2$ four-fermion operator is renormalised multiplicatively. The renormalisation adopted is non-perturbative, with a Schroedinger functional renormalisation condition. Renormalisation group running is also non-perturbative, up to very high energy scales. In one of the two tmQCD frameworks the computations have been performed at the physical $K$-meson mass, thus eliminating the need of mass extrapolations. Simulations have been performed at several lattice spacings and the continuum limit was reached by combining results from both tmQCD regularisations. Finite volume effects have been partially checked and turned out to be small. Exploratory studies have also been performed with non-degenerate valence flavours. The final result for the RGI bag parameter, with all sources of uncertainty (except quenching) under control, is $\hat B_K =0.789 \pm 0.046$.The B K parameter is computed in quenched lattice QCD with Wilson twisted mass fermions. Two variants of tmQCD are used; in both of them the relevant Δ S = 2 four-fermion operator is renormalised multiplicatively. The renormalisation adopted is non-perturbative, with a Schrödinger functional renormalisation condition. Renormalisation group running is also non-perturbative, up to very high energy scales. In one of the two tmQCD frameworks the computations have been performed at the physical K -meson mass, thus eliminating the need of mass extrapolations. Simulations have been performed at several lattice spacings and the continuum limit was reached by combining results from both tmQCD regularisations. Finite volume effects have been partially checked and turned out to be small. Exploratory studies have also been performed with non-degenerate valence flavours. The final result for the RGI bag parameter, with all sources of uncertainty (except quenching) under control, is B ˆ K = 0.789 ± 0.046 .The $B_K$ parameter is computed in quenched lattice QCD with Wilson twisted mass fermions. Two variants of tmQCD are used/ in both of them the relevant $\Delta S = 2$ four-fermion operator is renormalised multiplicatively. The renormalisation adopted is non-perturbative, with a Schroedinger functional renormalisation condition. Renormalisation group running is also non-perturbative, up to very high energy scales. In one of the two tmQCD frameworks the computations have been performed at the physical $K$-meson mass, thus eliminating the need of mass extrapolations. Simulations have been performed at several lattice spacings and the continuum limit was reached by combining results from both tmQCD regularisations. Finite volume effects have been partially checked and turned out to be small. Exploratory studies have also been performed with non-degenerate valence flavours. The final result for the RGI bag parameter, with all sources of uncertainty (except quenching) under control, is $\hat B_K =0.789 \pm 0.046$.hep-ph/0601002ROM2F-2005-27MS-TP-05-37CERN-PH-TH-2005-268FTUAM-05-20IFT-UAM-CSIC-05-55DESY-05-259CERN-PH-TH-2005-268FTUAM-2005-20MS-TP-2005-37ROM-2F-2005-27oai:cds.cern.ch:9194842005-12-31
spellingShingle Particle Physics - Phenomenology
Dimopoulos, P.
Heitger, J.
Palombi, F.
Pena, C.
Sint, S.
Vladikas, A.
A Precise determination of B(K) in quenched QCD
title A Precise determination of B(K) in quenched QCD
title_full A Precise determination of B(K) in quenched QCD
title_fullStr A Precise determination of B(K) in quenched QCD
title_full_unstemmed A Precise determination of B(K) in quenched QCD
title_short A Precise determination of B(K) in quenched QCD
title_sort precise determination of b(k) in quenched qcd
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.nuclphysb.2006.04.033
http://cds.cern.ch/record/919484
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