2013/07/31 by M. Hayakawa, K.-I. Ishikawa, K. -I. Ishikawa +3 · 19 citations
Mathematics · Physics and Astronomy · #Combinatorics #Coupling constant #Dimension (graph theory) #Dirac fermion #Electroweak interaction #Fermion #Gauge theory #Lattice (music) #Lattice gauge theory #Massless particle #Mathematical physics #Mathematics #Neutrino Physics Research #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Symmetry breaking #hep-lat #hep-ph
paper · pdf · doi:10.1103/physrevd.88.094504
published in Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 88(9) (American Physical Society) · 38 pages, 9 figures. v2)Minor corrections, references added. Version to appear in PRD
arxiv created 2013/11/06 · openalex publication_date 2013/11/18 · arxiv updated 2013/11/27 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
In the exploration of viable models of dynamical electroweak symmetry breaking, it is essential to locate the lower end of the conformal window and know the mass anomalous dimensions there for a variety of gauge theories. We calculate, with the Schr"odinger functional scheme, the running coupling constant and the mass anomalous dimension of SU(2) gauge theory with six massless Dirac fermions in the fundamental representation. The calculations are performed on 64--244 lattices over a wide range of lattice bare couplings to take the continuum limit. The discretization errors for both quantities are removed perturbatively. We find that the running slows down and comes to a stop at 0.06\ensuremath\lesssim1/g2\ensuremath\lesssim0.15 where the mass anomalous dimension is estimated to be 0.26\ensuremath\lesssim\ensuremathγm*\ensuremath\lesssim0.74.