We present a general analysis of SU(3) breaking effects in the semi-inclusive tau hadronic width. The recent ALEPH measurements of the inclusive Cabibbo-suppressed decay width of the tau and several moments of its invariant mass distribution are used to determine the value of the strange quark mass. We obtain, in the scheme, m(s)(M-tau(2)) = (119 +/- 24) MeV to O(alpha(s)(3)), which corresponds to m(s)(1 GeV2) = (164 +/- 33) MeV; m(s)(4 GeV2) = (114 +/- 23) MeV
Tau lepton decays with open strangeness in the final state are measured with the Opal detector at LE...
The following sections are included: Hadronic τ Decays Leptonic Tau Decays Semileptonic Decays Searc...
Recent experimental improvements on K-decay data allow for a precise extraction of the strangeness-c...
We present a general analysis of SU(3) breaking effects in the semi-inclusive tau hadronic width. Th...
Quark mass corrections to the tau hadronic width play a significant role only for the strange quark....
Quark mass corrections to the tau hadronic width play a significant role only for the strange quark....
In this work radiative corrections in the total hadronic decay rate of the tau-lepton and some momen...
The first complete calculation of the quadratic quark mass correction to the correlator of the two c...
The mass of the strange quark is determined from SU(3)-breaking effects in the tau hadronic width. C...
The strange quark mass is extracted from a finite energy sum rule (FESR) analysis of the flavor-brea...
A very precise determination of V_us can be obtained from the semi-inclusive hadronic decay width of...
Recent progress in the determination of |V_us| employing strange hadronic tau-decay data are reporte...
15 páginas, 3 figuras, 2 tablas.-- arXiv:hep-ph/9804462v1The perturbative quark-mass corrections to ...
The perturbative quark-mass corrections to the tau hadronic width are analysed to O(alpha(s)(3)m(q)(...
The invariant-mass distribution of the hadronic state in tau-decay can be used for testing fundament...
Tau lepton decays with open strangeness in the final state are measured with the Opal detector at LE...
The following sections are included: Hadronic τ Decays Leptonic Tau Decays Semileptonic Decays Searc...
Recent experimental improvements on K-decay data allow for a precise extraction of the strangeness-c...
We present a general analysis of SU(3) breaking effects in the semi-inclusive tau hadronic width. Th...
Quark mass corrections to the tau hadronic width play a significant role only for the strange quark....
Quark mass corrections to the tau hadronic width play a significant role only for the strange quark....
In this work radiative corrections in the total hadronic decay rate of the tau-lepton and some momen...
The first complete calculation of the quadratic quark mass correction to the correlator of the two c...
The mass of the strange quark is determined from SU(3)-breaking effects in the tau hadronic width. C...
The strange quark mass is extracted from a finite energy sum rule (FESR) analysis of the flavor-brea...
A very precise determination of V_us can be obtained from the semi-inclusive hadronic decay width of...
Recent progress in the determination of |V_us| employing strange hadronic tau-decay data are reporte...
15 páginas, 3 figuras, 2 tablas.-- arXiv:hep-ph/9804462v1The perturbative quark-mass corrections to ...
The perturbative quark-mass corrections to the tau hadronic width are analysed to O(alpha(s)(3)m(q)(...
The invariant-mass distribution of the hadronic state in tau-decay can be used for testing fundament...
Tau lepton decays with open strangeness in the final state are measured with the Opal detector at LE...
The following sections are included: Hadronic τ Decays Leptonic Tau Decays Semileptonic Decays Searc...
Recent experimental improvements on K-decay data allow for a precise extraction of the strangeness-c...