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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.

how it is stated · asserted 1.00 read the record →

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arXiv ID0912.4699 (version 4)
Pith IDODN7XMLV, Pith's permanent record of this paper and its review
CitationAlexander Quintero Velez, Nils Carqueville. "Remarks on quiver gauge theories from open topological string theory." arXiv:0912.4699 (2009). https://pith.science/paper/ODN7XMLV
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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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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,162 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.07 · states limitation 0.07 · human participants 0.01 · controlled comparison 0.05 · randomized assignment 0.01 · states quantitative result 0.08 · compares with prior results 0.95 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v4. Results and the main claim are underlined; .

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

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
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

What kind of paper the classifier reports this is: theoretical result 0.98 · evidence from proof or derivation 1.00.

What was examined, and what was not

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  • full text
  • figures and tables
  • references and citing sentences
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  • P abstract
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  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

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.

Human review
How the literature uses it

5 arXiv papers cite this in 7 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 6 sentences without a confident label

Cites it as background 1 paper

What it cites · 30 sentences without a confident label

Uses the method or tool of 8 papers
  • 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

  • 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

  • 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
  • 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

  • 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

  • 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
Cites as background 14 papers

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