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Remarks on quiver gauge theories from open topological string theory
High Energy Physics - Theory · Submitted 23 Dec 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Then we show that it precisely reproduces the results of the method of brane tilings, without having to resort to any effective field theory computations.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We study effective quiver gauge theories arising from a stack of D3-branes on certain Calabi-Yau singularities. Our point of view is a first principle approach via open topological string theory. This means that we construct the natural A-infinity-structure of open string amplitudes in the associated D-brane category. Then we show that it precisely reproduces the results of the method of brane tilings, without having to resort to any effective field theory computations. In particular, we prove a general and simple formula for effective superpotentials.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study effective quiver gauge theories arising from a stack of D3-branes on certain Calabi-Yau singularities. | contribution 0.64 | 0.80 | 0.04 | asserted 0.95 |
| s1 | Our point of view is a first principle approach via open topological string theory. | method 0.93 | 0.58 | 0.04 | asserted 0.99 |
| s2 | This means that we construct the natural A-infinity-structure of open string amplitudes in the associated D-brane category. | method 0.97 | 0.82 | 0.06 | asserted 0.97 |
| s3 | Then we show that it precisely reproduces the results of the method of brane tilings, without having to resort to any effective field theory computations. | result 0.99 | 0.94 | 0.58 | asserted 1.00 |
| s4 | In particular, we prove a general and simple formula for effective superpotentials. | result 0.94 | 0.95 | 0.44 | asserted 1.00 |
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The paper
Original abstract
We study effective quiver gauge theories arising from a stack of D3-branes on certain Calabi-Yau singularities. Our point of view is a first principle approach via open topological string theory. This means that we construct the natural A-infinity-structure of open string amplitudes in the associated D-brane category. Then we show that it precisely reproduces the results of the method of brane tilings, without having to resort to any effective field theory computations. In particular, we prove a general and simple formula for effective superpotentials.
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How the literature uses it
5 arXiv papers cite this in 7 sentences
Papers citing it · 6 sentences without a confident label
Cites it as background 1 paper
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We also thank Alastair Craw for pointing out the reference [ref] , and Nils Carqueville and Alexander Quintero Velez for sending an earlier version of [ref] .
Exact Lefschetz fibrations associated with dimer models · Introduction · 0.81
What it cites · 30 sentences without a confident label
Uses the method or tool of 8 papers
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To construct the $$-structure, we first use the elegant method of [ref] to find the higher products on $^b((Z))$ and then extend [ref] it to branes in $^b_Z((X))$.
A Geometric Unification of Dualities · Introduction and summary · 0.80
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To construct the $$-structure, we first use the elegant method of [ref] to find the higher products on $^b((Z))$ and then extend [ref] it to branes in $^b_Z((X))$.
Sheaves on local Calabi-Yau varieties · Introduction and summary · 0.80
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To construct the $$-structure, we first use the elegant method of [ref] to find the higher products on $^b((Z))$ and then extend [ref] it to branes in $^b_Z((X))$.
Suspending Lefschetz fibrations, with an application to Local Mirror Symmetry · Introduction and summary · 0.80
Compares with 3 papers
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If we label the arrows as shown in [ref], then the brane tiling superpotential is [equation] where $ρ_1$, $ρ_2$ and $ρ_3$ are the deleted arrows corresponding to the perfect matching $π_10$; compare [ref] .
Toric Duality as Seiberg Duality and Brane Diamonds · An example: $dP_2$ · 0.80
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If we label the arrows as shown in [ref], then the brane tiling superpotential is [equation] where $ρ_1$, $ρ_2$ and $ρ_3$ are the deleted arrows corresponding to the perfect matching $π_10$; compare [ref] .
Seiberg duality as derived equivalence for some quiver gauge theories · An example: $dP_2$ · 0.80
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Finally, our proof differs from the one of [ref] in that we emphasise the role of the surface $Z$ and find the $$-structure on $^b_Z((X))$ by extending that of $^b((Z))$; to construct the latter we do not have to perform explicit calculations since we make use of Keller's higher multiplication theorem [ref] .
Exact Lefschetz fibrations associated with dimer models · Introduction and summary · 0.86
Cites as support 1 paper
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A result of [ref] provides an equivalence between $^b_Z((X))$ and $^b_0(A)$.
T-structures on some local Calabi-Yau varieties · The $A_∞$-structure of the D-brane category $𝐃^b_Z(Coh(X))$ · 0.96
Cites as background 14 papers
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In order to extract the data of the effective quiver gauge theory from the geometry of $Z$, several procedures have been developed in [ref] , most notably the fast inverse algorithm and the brane tiling method.
Properly ordered dimers, $R$-charges, and an efficient inverse algorithm · Introduction and summary · 0.85
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In order to extract the data of the effective quiver gauge theory from the geometry of $Z$, several procedures have been developed in [ref] , most notably the fast inverse algorithm and the brane tiling method.
D-Brane Gauge Theories from Toric Singularities and Toric Duality · Introduction and summary · 0.85
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In order to extract the data of the effective quiver gauge theory from the geometry of $Z$, several procedures have been developed in [ref] , most notably the fast inverse algorithm and the brane tiling method.
Phase Structure of D-brane Gauge Theories and Toric Duality · Introduction and summary · 0.85
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