2005/11/30 by Agostino Patella · 13 citations
Mathematics · Physics and Astronomy · #Antisymmetric relation #Black Holes and Theoretical Physics #Computer science #Equivalence (formal languages) #Gauge theory #Lattice (music) #Lattice gauge theory #Mass gap #Massless particle #Mathematical physics #Mathematics #Orientifold #Particle physics #Particle physics theoretical and experimental studies #Physics #Planar #Pure mathematics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #String theory #Theoretical physics #Wilson loop #hep-lat
paper · pdf · doi:10.1103/physrevd.74.034506
published in Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 74(3) (American Physical Society) · 14 pages, 3 EPS figures, uses REVTeX4
arxiv created 2006/04/21 · openalex publication_date 2006/08/09 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
In a recent paper, Armoni, Shifman, and Veneziano (ASV) gave a formal nonperturbative proof of planar equivalence between the bosonic sectors of SU(N) super Yang-Mills theory and of a gauge theory with a massless quark in the antisymmetric two-indexes representation. In the case of three colors, the latter theory is nothing but one-flavor QCD. I will give a lattice version of the ASV proof of orientifold planar equivalence. It will be clear that it holds only in the strong-coupling and large-mass phase. Therefore, numerical simulations are necessary to test the validity of the orientifold planar equivalence in a physical region of the bare parameters on the lattice and to estimate the size of 1/N corrections.