Refining the Proof of Planar Equivalence

We outline a full non-perturbative proof of planar (large-N) equivalence between bosonic correlators in a theory with Majorana fermions in the adjoint representation and one with Dirac fermions in the two-index (anti)symmetric representation. In a particular case (one flavor), this reduces to our pr...

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Detalles Bibliográficos
Autores principales: Armoni, A., Shifman, M., Veneziano, G.
Lenguaje:eng
Publicado: 2004
Materias:
Particle Physics - Theory
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.71.045015
http://cds.cern.ch/record/811729
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author Armoni, A.
Shifman, M.
Veneziano, G.
author_facet Armoni, A.
Shifman, M.
Veneziano, G.
author_sort Armoni, A.
collection CERN
description We outline a full non-perturbative proof of planar (large-N) equivalence between bosonic correlators in a theory with Majorana fermions in the adjoint representation and one with Dirac fermions in the two-index (anti)symmetric representation. In a particular case (one flavor), this reduces to our previous result - planar equivalence between super-Yang--Mills theory and a non-supersymmetric ``orientifold field theory.'' The latter theory becomes one-flavor massless QCD at N=3.
id cern-811729
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2004
record_format invenio
spelling cern-8117292023-03-14T18:16:13Zdoi:10.1103/PhysRevD.71.045015http://cds.cern.ch/record/811729engArmoni, A.Shifman, M.Veneziano, G.Refining the Proof of Planar EquivalenceParticle Physics - TheoryWe outline a full non-perturbative proof of planar (large-N) equivalence between bosonic correlators in a theory with Majorana fermions in the adjoint representation and one with Dirac fermions in the two-index (anti)symmetric representation. In a particular case (one flavor), this reduces to our previous result - planar equivalence between super-Yang--Mills theory and a non-supersymmetric ``orientifold field theory.'' The latter theory becomes one-flavor massless QCD at N=3.We outline a full non-perturbative proof of planar (large-N) equivalence between bosonic correlators in a theory with Majorana fermions in the adjoint representation and one with Dirac fermions in the two-index (anti)symmetric representation. In a particular case (one flavor), this reduces to our previous result - planar equivalence between super-Yang--Mills theory and a non-supersymmetric ``orientifold field theory.'' The latter theory becomes one-flavor massless QCD at N=3.hep-th/0412203CERN-PH-TH-2004-248SWAT-421FTPI-MINN-04-33UMN-TH-2320-04CERN-PH-TH-2004-248SWAT-421FTPI-MINN-2004-33UMN-TH-2320oai:cds.cern.ch:8117292004-12-17
spellingShingle Particle Physics - Theory
Armoni, A.
Shifman, M.
Veneziano, G.
Refining the Proof of Planar Equivalence
title Refining the Proof of Planar Equivalence
title_full Refining the Proof of Planar Equivalence
title_fullStr Refining the Proof of Planar Equivalence
title_full_unstemmed Refining the Proof of Planar Equivalence
title_short Refining the Proof of Planar Equivalence
title_sort refining the proof of planar equivalence
topic Particle Physics - Theory
url https://dx.doi.org/10.1103/PhysRevD.71.045015
http://cds.cern.ch/record/811729
work_keys_str_mv AT armonia refiningtheproofofplanarequivalence
AT shifmanm refiningtheproofofplanarequivalence
AT venezianog refiningtheproofofplanarequivalence

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