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On Realising N=1 Super Yang-Mills in M theory
High Energy Physics - Theory · Submitted 10 Nov 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Pure N=1 super Yang-Mills theory can be realised as a certain low energy limit of M theory near certain singularities in $G_2$-holonomy spaces.
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Pure N=1 super Yang-Mills theory can be realised as a certain low energy limit of M theory near certain singularities in $G_2$-holonomy spaces. For SU(n) and SO(2n) gauge groups these $M$ theory backgrounds can be regarded as strong coupling limits of wrapped D6-brane configurations in Type IIA theory on certain non-compact Calabi-Yau spaces such as the deformed conifold. Various aspects of such realisations are studied including the generation of the superpotential, domain walls, QCD strings and the relation to recent work of Vafa. In the spirit of this recent work we propose a `gravity dual' of M theory near these singularities.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Pure N=1 super Yang-Mills theory can be realised as a certain low energy limit of M theory near certain singularities in $G_2$-holonomy spaces. | background 0.44 | 0.26 | 0.64 | asserted 1.00 |
| s1 | For SU(n) and SO(2n) gauge groups these $M$ theory backgrounds can be regarded as strong coupling limits of wrapped D6-brane configurations in Type IIA theory on certain non-compact Calabi-Yau spaces such as the deformed conifold. | interpretation 0.42 | 0.30 | 0.13 | asserted 0.60 |
| s2 | Various aspects of such realisations are studied including the generation of the superpotential, domain walls, QCD strings and the relation to recent work of Vafa. | contribution 0.99 | 0.79 | 0.11 | asserted 0.97 |
| s3 | In the spirit of this recent work we propose a `gravity dual' of M theory near these singularities. | contribution 0.99 | 0.81 | 0.26 | speculative 0.66 |
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Original abstract
Pure N=1 super Yang-Mills theory can be realised as a certain low energy limit of M theory near certain singularities in $G_2$-holonomy spaces. For SU(n) and SO(2n) gauge groups these $M$ theory backgrounds can be regarded as strong coupling limits of wrapped D6-brane configurations in Type IIA theory on certain non-compact Calabi-Yau spaces such as the deformed conifold. Various aspects of such realisations are studied including the generation of the superpotential, domain walls, QCD strings and the relation to recent work of Vafa. In the spirit of this recent work we propose a `gravity dual' of M theory near these singularities.
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References
How the literature uses it
44 arXiv papers cite this in 64 sentences
Papers citing it · 43 sentences without a confident label
Builds on it 1 paper
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In analogy to the open string transition discussed in [ref] , we expect the gravitational version to replace the strongly coupled 9-brane by some flux.
Non-perturbative Resolution of Strong Coupling Singularities in 4d N=1 Heterotic/M-theory · Conclusions · 0.90
Cites it as support 1 paper
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Since theories with no normalizable zero modes have a mass gap, the smooth interpolation between such theories and non-abelian supersymmetric gauge theories has been viewed as evidence supporting the statement that non-abelian supersymmetric gauge theories have a mass gap [ref] .
The String Landscape: On Formulas for Counting Vacua · Introduction · 0.96
Cites it as background 16 papers
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We begin with a short review of the original $M$-theory flop and its reduction to type IIA string theory [ref] .
New $G_2$-conifolds in $M$-theory and their Field Theory Interpretation · Models for codimension four singularities and the $M$-theory flop · 0.97
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In M-theory compactified on a singular $G_2$ holonomy manifold $X$, non-Abelian gauge fields live in $R^3,1×Q$ where $Q∈X$ is an associative three-cycle along which there is an orbifold singularity of A-D-E type [ref] , [ref] , [ref] , [ref] , [ref] .
Scanning the Fluxless $G_2$ Landscape · Threshold corrections · 0.96
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Recall that in the compactifications we study here, non-Abelian gauge fields arise from co-dimension four singularities [ref] , [ref] , [ref] , [ref] , [ref] .
Kahler Independence of the G2-MSSM · Moduli stabilization · 0.93
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