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An M-theory Flop as a Large N Duality
High Energy Physics - Theory · Submitted 28 Nov 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show how a recently proposed large $N$ duality in the context of type IIA strings with ${\cal N}=1$ supersymmetry in 4 dimensions can be derived from purely geometric considerations by embedding type IIA strings in M-theory.
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We show how a recently proposed large $N$ duality in the context of type IIA strings with ${\cal N}=1$ supersymmetry in 4 dimensions can be derived from purely geometric considerations by embedding type IIA strings in M-theory. The phase structure of M-theory on $G_2$ holonomy manifolds and an $S^3$ flop are the key ingredients in this derivation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We show how a recently proposed large $N$ duality in the context of type IIA strings with ${\cal N}=1$ supersymmetry in 4 dimensions can be derived from purely geometric considerations by embedding type IIA strings in M-theory. | contribution 0.82 | 0.93 | 0.86 | asserted 1.00 |
| s1 | The phase structure of M-theory on $G_2$ holonomy manifolds and an $S^3$ flop are the key ingredients in this derivation. | method 0.90 | 0.49 | 0.12 | asserted 1.00 |
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The paper
Original abstract
We show how a recently proposed large $N$ duality in the context of type IIA strings with ${\cal N}=1$ supersymmetry in 4 dimensions can be derived from purely geometric considerations by embedding type IIA strings in M-theory. The phase structure of M-theory on $G_2$ holonomy manifolds and an $S^3$ flop are the key ingredients in this derivation.
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References
How the literature uses it
39 arXiv papers cite this in 60 sentences
Papers citing it · 37 sentences without a confident label
Builds on it 2 papers
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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
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It should also be interesting to extend all this story to the type II A case, using backgrounds like the ones in [ref] .
Elaborations on the String Dual to N=1 SQCD · Summary, conclusions and future directions · 0.88
Compares with it 3 papers
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Notice that this is different from the closely related setup in [ref] , where the relevant geometric transition involved D6 branes wrapped in the conifold, although this was embedded in the $G_2$ holonomy context by uplifting to M-theory.
Fivebranes and resolved deformed G_2 manifolds · Summary · 0.95
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This is in contrast to the similar transition involving D6 branes on the $S^3$ of the deformed conifold [ref] which requires some non-geometric insight.
The unwarped, resolved, deformed conifold: fivebranes and the baryonic branch of the Klebanov-Strassler theory · Introduction · 1.00
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Notice that a similar replacement of a D-brane gauge theory by a closed string gauge theory has been discussed previously in the context of Type IIA/M-theory compactifications in [ref] .[Another example of a gauge theory having a perturbative closed string origin before and a brane origin after a smooth transition has recently been discussed in 4d $=2$ compactifications of the heterotic string in [ref] .]
Towards the Non-Perturbative Completion of 4d N=1 Effective Theories of Gravity · Missing, massive degrees of freedom · 0.81
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 15 papers
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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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This setup was discussed in [ref] .
The quark-gluon plasma and D6-branes on the conifold · M-theory on the $G_2$ holonomy manifoldM-theory on the G2 holonomy manifold · 0.92
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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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