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Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD

We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a phys...

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Detalles Bibliográficos
Autores principales: Dimopoulos, P., Heitger, J., Palombi, F., Pena, C., Sint, S., Vladikas, A.
Lenguaje:eng
Publicado: 2007
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2007.03.051
http://cds.cern.ch/record/1016554
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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 We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking effects, which are at most 5%, decrease as we approach the continuum limit. We also compute the pseudoscalar decay constant in the continuum limit, with reduced systematics. As a consequence of improved tuning of the mass parameters at $\beta = 6.1$, we reanalyse our previous $B_K$ results. Our main phenomenological findings are $r_0 f_K = 0.421(7)$ and $\hat B_K = 0.735(71)$.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-10165542023-04-14T03:07:37Zdoi:10.1016/j.nuclphysb.2007.03.051http://cds.cern.ch/record/1016554engDimopoulos, P.Heitger, J.Palombi, F.Pena, C.Sint, S.Vladikas, A.Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCDParticle Physics - LatticeWe simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking effects, which are at most 5%, decrease as we approach the continuum limit. We also compute the pseudoscalar decay constant in the continuum limit, with reduced systematics. As a consequence of improved tuning of the mass parameters at $\beta = 6.1$, we reanalyse our previous $B_K$ results. Our main phenomenological findings are $r_0 f_K = 0.421(7)$ and $\hat B_K = 0.735(71)$.We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking effects, which are at most 5%, decrease as we approach the continuum limit. We also compute the pseudoscalar decay constant in the continuum limit, with reduced systematics. As a consequence of improved tuning of the mass parameters at $\beta = 6.1$, we reanalyse our previous $B_K$ results. Our main phenomenological findings are $r_0 f_K = 0.421(7)$ and $\hat B_K = 0.735(71)$.We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking effects, which are at most 5%, decrease as we approach the continuum limit. We also compute the pseudoscalar decay constant in the continuum limit, with reduced systematics. As a consequence of improved tuning of the mass parameters at $\beta = 6.1$, we reanalyse our previous $B_K$ results. Our main phenomenological findings are $r_0 f_K = 0.421(7)$ and $\hat B_K = 0.735(71)$.We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking effects, which are at most 5%, decrease as we approach the continuum limit. We also compute the pseudoscalar decay constant in the continuum limit, with reduced systematics. As a consequence of improved tuning of the mass parameters at β = 6.1 , we reanalyze our previous B K results. Our main phenomenological findings are r 0 f K = 0.421 ( 7 ) and B ˆ K = 0.735 ( 71 ) .hep-lat/0702017ROM2F-2007-03MS-TP-07-1CERN-PH-TH-2007-018MKPH-T-07-03TRINLAT-07-03CERN-PH-TH-2007-018MKPH-T-2007-03MS-TP-2007-1ROM-2F-2007-03oai:cds.cern.ch:10165542007-02-13
spellingShingle Particle Physics - Lattice
Dimopoulos, P.
Heitger, J.
Palombi, F.
Pena, C.
Sint, S.
Vladikas, A.
Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD
title Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD
title_full Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD
title_fullStr Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD
title_full_unstemmed Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD
title_short Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD
title_sort flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass qcd
topic Particle Physics - Lattice
url https://dx.doi.org/10.1016/j.nuclphysb.2007.03.051
http://cds.cern.ch/record/1016554
work_keys_str_mv AT dimopoulosp flavoursymmetryrestorationandkaonweakmatrixelementsinquenchedtwistedmassqcd
AT heitgerj flavoursymmetryrestorationandkaonweakmatrixelementsinquenchedtwistedmassqcd
AT palombif flavoursymmetryrestorationandkaonweakmatrixelementsinquenchedtwistedmassqcd
AT penac flavoursymmetryrestorationandkaonweakmatrixelementsinquenchedtwistedmassqcd
AT sints flavoursymmetryrestorationandkaonweakmatrixelementsinquenchedtwistedmassqcd
AT vladikasa flavoursymmetryrestorationandkaonweakmatrixelementsinquenchedtwistedmassqcd