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Wall Crossing and M-theory
High Energy Physics - Theory · Submitted 8 Aug 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The generating function of the D-brane bound states is expressed as a reduction of the square of the topological string partition function, in all chambers of the Kahler moduli space.
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The abstract, sentence by sentence
We study BPS bound states of D0 and D2 branes on a single D6 brane wrapping a Calabi-Yau 3-fold X. When X has no compact 4-cyles, the BPS bound states are organized into a free field Fock space, whose generators correspond to BPS states of spinning M2 branes in M-theory compactified down to 5 dimensions by a Calabi-Yau 3-fold X. The generating function of the D-brane bound states is expressed as a reduction of the square of the topological string partition function, in all chambers of the Kahler moduli space.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study BPS bound states of D0 and D2 branes on a single D6 brane wrapping a Calabi-Yau 3-fold X. | contribution 0.96 | 0.86 | 0.07 | asserted 0.95 |
| s1 | When X has no compact 4-cyles, the BPS bound states are organized into a free field Fock space, whose generators correspond to BPS states of spinning M2 branes in M-theory compactified down to 5 dimensions by a Calabi-Yau 3-fold X. | result 0.91 | 0.65 | 0.26 | asserted 1.00 |
| s2 | The generating function of the D-brane bound states is expressed as a reduction of the square of the topological string partition function, in all chambers of the Kahler moduli space. | result 0.94 | 0.84 | 0.44 | asserted 1.00 |
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The paper
Original abstract
We study BPS bound states of D0 and D2 branes on a single D6 brane wrapping a Calabi-Yau 3-fold X. When X has no compact 4-cyles, the BPS bound states are organized into a free field Fock space, whose generators correspond to BPS states of spinning M2 branes in M-theory compactified down to 5 dimensions by a Calabi-Yau 3-fold X. The generating function of the D-brane bound states is expressed as a reduction of the square of the topological string partition function, in all chambers of the Kahler moduli space.
Human review
References
How the literature uses it
36 arXiv papers cite this in 79 sentences
Papers citing it · 52 sentences without a confident label
Builds on it 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.
M theory and the Coulomb phase of higher rank DT invariants · Introduction · 1.00
Compares with it 2 papers
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[This is reminiscent of the situation in [ref] , where the analysis was simplified by moving to the locus where all the phases of central charges of the D2-D0 particles align.]
BPS Graphs: From Spectral Networks to BPS Quivers · Definition · 0.91
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The first factor in ([ref]) is strongly reminiscent of the partition function of (framed) Donaldson-Thomas invariants of the conifold [ref] .
Gluing two affine Yangians of $\mathfrak{gl}_1$ · Geometric interpretation of framing and shifting via BPS partition function · 0.84
Cites it as background 20 papers
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In this section we will review the work in [ref] .
M theory and the Coulomb phase of higher rank DT invariants · Preliminaries · 0.91
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The closed BPS partition function for generalized conifolds is studied in [ref] .
The Non-commutative Topological Vertex and Wall Crossing Phenomena · Closed BPS Invariants · 0.86
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In section [ref], we review the basic idea of [ref] .
Open BPS Wall Crossing and M-theory · Introduction · 0.94
What it cites · 32 sentences without a confident label
Builds on 2 papers
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In this paper we will generalize the results of [ref] to include the background dependence of the M-theory computation.
M-theory and a Topological String Duality · Introduction · 1.00
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In this final section, we point out that our M-theory viewpoint discussed in this paper allows us to derive, in the present context of D6, D2 and D0 degeneracies, the “semi-primitive" wall crossing formula of [ref] .
Split States, Entropy Enigmas, Holes and Halos · Relation to the Denef-Moore formula · 0.87
Uses data or values from 3 papers
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The topological string partition function is given by [ref] _top(q,Q_1,Q_2)=M(q) ( ∏_n=1^∞ (1-Q_1 q^n)^n ) ∏_k,n=1^∞ ( (1-q^n Q_1 Q_2^k ) (1-q^n Q_1^-1 Q_2^k)/(1-q^n-1 Q_2^k) (1-q^n+1 Q_2^k) )^n where $Q_1$ and $Q_2$ are the variables corresponding to $β_1$ and $β_2$.
Matrix Models, Geometric Engineering and Elliptic Genera · A Non-toric Example · 0.83
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N_β=±1^0=1, N_β=0^0=-2, and that all BPS states in 5 dimensions has no intrinsic spin [ref] .
M-Theory and Topological Strings--I · Resolved conifold · 0.93
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N_β=±1^0=1, N_β=0^0=-2, and that all BPS states in 5 dimensions has no intrinsic spin [ref] .
M-Theory and Topological Strings--II · Resolved conifold · 0.93
Compares with 5 papers
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These agree with the results in [ref] in all chambers.
Non-commutative Donaldson-Thomas theory and the conifold · Resolved conifold · 0.97
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These agree with the results in [ref] in all chambers.
Counting invariant of perverse coherent sheaves and its wall-crossing · Resolved conifold · 0.97
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These agree with the results in [ref] in all chambers.
Wall crossing in local Calabi Yau manifolds · Resolved conifold · 0.97
Cites as background 9 papers
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The relation between the GV invariants and DT invariants was suggested and formulated in [ref] , and its physical explanation was given in [ref] using the 4D/5D connection [ref] .
Quantum Foam and Topological Strings · Introduction · 0.84
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The relation between the GV invariants and DT invariants was suggested and formulated in [ref] , and its physical explanation was given in [ref] using the 4D/5D connection [ref] .
New Connections Between 4D and 5D Black Holes · Introduction · 0.84
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The relation between the GV invariants and DT invariants was suggested and formulated in [ref] , and its physical explanation was given in [ref] using the 4D/5D connection [ref] .
M-theory and a Topological String Duality · Introduction · 0.84
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