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M theory and the Coulomb phase of higher rank DT invariants
High Energy Physics - Theory · Submitted 11 Apr 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In this paper, we advance an M theory model corresponding to the Coulomb phase of higher rank Donaldson-Thomas(DT) invariants.
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The abstract, sentence by sentence
In this paper, we advance an M theory model corresponding to the Coulomb phase of higher rank Donaldson-Thomas(DT) invariants.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this paper, we advance an M theory model corresponding to the Coulomb phase of higher rank Donaldson-Thomas(DT) invariants. | contribution 1.00 | 0.90 | 0.48 | asserted 1.00 |
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The paper
Original abstract
In this paper, we advance an M theory model corresponding to the Coulomb phase of higher rank Donaldson-Thomas(DT) invariants.
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How the literature uses it
1 arXiv paper cite this in 1 sentence
What it cites · 33 sentences without a confident label
Builds on 1 paper
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In Section 3 we will generalize [ref] to the multi D6-brane case and propose a formula corresponding to the Coulomb phase of higher rank DT invariants.
Wall Crossing and M-theory · Introduction · 1.00
Uses the method or tool of 5 papers
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Thus we can use the equivariant cohomology technique to construct a quiver matrix model and calculate the contribution of instantons [ref] .
Topological Quiver Matrix Models and Quantum Foam · Coulomb phase of higher rank DT invariants on multi D6-branes · 0.99
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Thus we can use the equivariant cohomology technique to construct a quiver matrix model and calculate the contribution of instantons [ref] .
Cohomological gauge theory, quiver matrix models and Donaldson-Thomas theory · Coulomb phase of higher rank DT invariants on multi D6-branes · 0.99
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Thus we can use the equivariant cohomology technique to construct a quiver matrix model and calculate the contribution of instantons [ref] .
Quiver Matrix Model and Topological Partition Function in Six Dimensions · Coulomb phase of higher rank DT invariants on multi D6-branes · 0.99
Compares with 2 papers
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So according to the equation ([ref]) we have [equation] which is same as the results in [ref] .
Cohomological gauge theory, quiver matrix models and Donaldson-Thomas theory · $^3$ · 0.95
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So according to the equation ([ref]) we have [equation] which is same as the results in [ref] .
Quantum Foam and Topological Strings · $^3$ · 0.95
Cites as background 15 papers
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In this section we will review the work in [ref] .
Wall Crossing and M-theory · Preliminaries · 0.91
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But for the higher rank DT invariants, which are known to be the degeneracies of D0 and D2-branes bound to multiple D6-branes wrapped on Calabi-Yau threefolds, we only know few details [ref] .
Cohomological gauge theory, quiver matrix models and Donaldson-Thomas theory · Introduction · 0.83
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But for the higher rank DT invariants, which are known to be the degeneracies of D0 and D2-branes bound to multiple D6-branes wrapped on Calabi-Yau threefolds, we only know few details [ref] .
On a computation of rank two Donaldson-Thomas invariants · Introduction · 0.83
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