2017/08/31 by Shoichi Sasaki
Physics and Astronomy · #Atomic and Subatomic Physics Research #Baryon #Hyperon #Lattice (music) #Lepton #Meson #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Physics #Pseudovector #Quantum Chromodynamics and Particle Interactions #Semileptonic decay #hep-lat #hep-ph
paper · pdf · doi:10.1103/physrevd.96.074509
published as Phys. Rev. D 96, 074509 (2017) · 17 pages, 20 figures; v2: version published in PRD
openalex created_date 2017/08/31 · openalex publication_date 2017/10/25 · arxiv created 2017/10/26 · arxiv updated 2017/10/27 · openalex updated_date 2026/08/05
We determine the hyperon vector couplings f1(0) for \mathrm\ensuremathΣ^\ensuremath-\ensuremath→nl^\ensuremath-\ensuremathνl and \mathrm\ensuremathΞ0\ensuremath→\mathrm\ensuremathΣ+l^\ensuremath-\ensuremathνl semileptonic decays in the continuum limit with (2+1)-flavors of dynamical domain-wall fermions, using the Iwasaki gauge action at two different lattice spacings of a=0.114(2) and 0.086(2) fm. A theoretical estimation of flavor SU(3)-breaking effect on the vector coupling is required to extract Vus from the experimental rate of hyperon beta decays. We obtain the vector couplings f1(0) for \mathrm\ensuremathΣ\ensuremath→N and \mathrm\ensuremathΞ\ensuremath→\mathrm\ensuremathΣ beta-decays with an accuracy of less than one percent. We then find that lattice results of f1(0) combined with the best estimate of |Vus| with imposing Cabibbo-Kobayashi-Maskawa (CKM) unitarity are slightly deviated from the experimental result of |Vusf1(0)| for the \mathrm\ensuremathΣ\ensuremath→N beta-decay. This discrepancy can be attributed to an assumption made in the experimental analysis on |Vusf1(0)|, where the induced second-class form factor g2 is set to be zero regardless of broken SU(3) symmetry. We report on this matter and then estimate the possible value of g2(0), which is evaluated from the experimental decay rate with our lattice result of f1(0) under the first-row CKM-unitarity condition.