2008/11/20 by Yoshio Kikukawa, Fumihiko Sugino · 23 citations
Mathematics · Physics and Astronomy · #Black Holes and Theoretical Physics #Gauge theory #Hamiltonian lattice gauge theory #Holomorphic function #Lattice (music) #Lattice QCD #Lattice field theory #Lattice model (finance) #Mathematical physics #Mathematics #Particle physics #Particle physics theoretical and experimental studies #Physics #Pure mathematics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Supercharge #Superpotential #Supersymmetry #Theoretical physics #hep-lat #hep-th
paper · pdf · doi:10.1016/j.nuclphysb.2009.04.007
published in Nuclear Physics B 819(1-2), 76-115 (Elsevier BV) · 46 pages, no figure; (v2) references added; (v3) typos corrected
arxiv created 2008/11/20 · openalex publication_date 2009/04/18 · arxiv updated 2009/12/01 · openalex created_date 2019/07/30 · openalex updated_date 2026/08/05
In this paper, we introduce the overlap Dirac operator, which satisfies the Ginsparg-Wilson relation, to the matter sector of two-dimensional N=(2,2) lattice supersymmetric QCD (SQCD) with preserving one of the supercharges. It realizes the exact chiral flavor symmetry on the lattice, to make possible to define the lattice action for general number of the flavors of fundamental and anti-fundamental matter multiplets and for general twisted masses. Furthermore, superpotential terms can be introduced with exact holomorphic or anti-holomorphic structure on the lattice. We also consider the lattice formulation of matter multiplets charged only under the central U(1) (the overall U(1)) of the gauge group G=U(N), and then construct lattice models for gauged linear sigma models with exactly preserving one supercharge and their chiral flavor symmetry.