An insight on the Proof of Orientifold Planar Equivalence on the Lattice
arXiv:hep-lat/0511037 · doi:10.1103/PhysRevD.74.034506
Abstract
In a recent paper, Armoni, Shifman and Veneziano (ASV) gave a formal non-perturbative 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. Numerical simulations are necessary to test the validity of that proof and to estimate the size of 1/N corrections. As a first step towards numerical simulations, I will give a lattice version of the ASV proof of orientifold planar equivalence in the strong-coupling and large-mass phase.
14 pages, 3 EPS figures, uses REVTeX4
References in corpus (5)
- Exact Results in Non-Supersymmetric Large N Orientifold Field Theories
- SUSY Relics in One-Flavor QCD from a New 1/N Expansion
- Refining the Proof of Planar Equivalence
- Non-perturbative equivalences among large N gauge theories with adjoint and bifundamental matter fields
- QCD Quark Condensate from SUSY and the Orientifold Large-N Expansion
Cited by in corpus (12)
- (In)validity of large N orientifold equivalence
- Quark condensate in two-flavor QCD
- Quark condensate in one-flavor QCD
- Lattice Study of Planar Equivalence: The Quark Condensate
- A note on C-Parity Conservation and the Validity of Orientifold Planar Equivalence
- A numerical investigation of orientifold planar equivalence for quenched mesons
- Center symmetry and the orientifold planar equivalence
- Spectrum of orientifold QCD in the strong coupling and hopping expansion approximation
- Domain Walls and Metastable Vacua in Hot Orientifold Field Theories
- The one-flavor quark condensate and related problems
- Orientifold Planar Equivalence: The Chiral Condensate
- About Orientifold Planar Equivalence on the Lattice