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Attractors and the Holomorphic Anomaly
High Energy Physics - Theory · Submitted 14 Dec 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our analysis results in a generalized formula for the relation between the microscopic density of black hole states and topological strings valid for all backgrounds.
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The abstract, sentence by sentence
Motivated by the recently proposed connection between N=2 BPS black holes and topological strings, I study the attractor equations and their interplay with the holomorphic anomaly equation. The topological string partition function is interpreted as a wave-function obtained by quantizing the real cohomology of the Calabi-Yau. In this interpretation the apparent background dependence due to the holomorphic anomaly is caused by the choice of complex polarization. The black hole attractor equations express the moduli in terms of the electric and magnetic charges, and lead to a real polarization in which the background dependence disappears. Our analysis results in a generalized formula for the relation between the microscopic density of black hole states and topological strings valid for all backgrounds.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Motivated by the recently proposed connection between N=2 BPS black holes and topological strings, I study the attractor equations and their interplay with the holomorphic anomaly equation. | contribution 0.74 | 0.85 | 0.04 | asserted 0.72 |
| s1 | The topological string partition function is interpreted as a wave-function obtained by quantizing the real cohomology of the Calabi-Yau. | interpretation 0.48 | 0.55 | 0.06 | asserted 1.00 |
| s2 | In this interpretation the apparent background dependence due to the holomorphic anomaly is caused by the choice of complex polarization. | interpretation 0.94 | 0.55 | 0.21 | asserted 1.00 |
| s3 | The black hole attractor equations express the moduli in terms of the electric and magnetic charges, and lead to a real polarization in which the background dependence disappears. | result 0.49 | 0.60 | 0.25 | asserted 1.00 |
| s4 | Our analysis results in a generalized formula for the relation between the microscopic density of black hole states and topological strings valid for all backgrounds. | result 0.98 | 0.95 | 0.78 | asserted 1.00 |
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Original abstract
Motivated by the recently proposed connection between N=2 BPS black holes and topological strings, I study the attractor equations and their interplay with the holomorphic anomaly equation. The topological string partition function is interpreted as a wave-function obtained by quantizing the real cohomology of the Calabi-Yau. In this interpretation the apparent background dependence due to the holomorphic anomaly is caused by the choice of complex polarization. The black hole attractor equations express the moduli in terms of the electric and magnetic charges, and lead to a real polarization in which the background dependence disappears. Our analysis results in a generalized formula for the relation between the microscopic density of black hole states and topological strings valid for all backgrounds.
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References
How the literature uses it
12 arXiv papers cite this in 20 sentences
Papers citing it · 15 sentences without a confident label
Cites it as background 5 papers
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First, let us recall the wave function interpretation of the topological string partition function, following [ref] .
Revisiting the Quantum Geometry of Torus-fibered Calabi-Yau Threefolds · Wave-function property of the topological string partition function · 0.91
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This review section is based on [ref] .
Geometric Transition as a Change of Polarization · Wavefuncion interpretation of closed topological strings · 0.98
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These advances have also led to much progress in our understanding of the topological string amplitude, in particular with regard to its wave function character [ref] .
Topological wave functions and the 4D-5D lift · Introduction · 0.86
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