The Spectrum of $BPS$ Branes on a Noncompact Calabi-Yau
By Michael R Douglas, B. Fiol, Christian Romelsberger. 2000
179 citations recorded by the source corpus.
We begin the study of the spectrum of BPS branes and its variation on lines of marginal stability on 2(?3), a Calabi-Yau ALE space asymptotic to 3/3. We show how to get the complete spectrum near the large volume limit and near the orbifold point, and find a striking similarity between the descriptions of holomorphic bundles and BPS branes in these two limits. We use these results to develop a general picture of the spectrum. We also suggest a generalization of some of the ideas to the quintic Calabi-Yau.
Subfields: Geometry and Topology, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/dfde3063b09f03112558293e51f33be6ba836694
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In Geometry and Topology
- M. Graña
- A. Kapustin
- G. Moore
- P. Aspinwall
- T. Bridgeland
- Yukinobu Toda
- Clay Córdova
- Michael R Douglas
In Nuclear and High Energy Physics
In Statistical and Nonlinear Physics
Citations in the corpus
- Dirichlet Branes and Mirror Symmetry (2009, methodology): “Thus, we can get a quite explicit picture in this case, studied in [138, 137, 149].”
- D-Branes on Calabi-Yau Manifolds (2004, methodology): “he example is C3/Z 3 where ggenerates Z 3 and acts as g: (z 1,z 2,z 3) →(ωz 1,ωz 2,ωz 3) for ω= exp(2πi/3). Much of the analysis of D-branes on orbifolds has been done in this simplest example (e.g., [118,157,159,175]). Let Vi, i= 0,...,2 be the one-dimensional irreducible representations of Z 3 giv”
- $\mathcal{N} = 2$ quantum field theories and their BPS quivers (2011, background): “Fractional branes as a basis of BPS quivers were studied in [26, 29, 30].”
- A scan for new N = 1 vacua on twisted tori (2006, background): “o show that the D–term BPS conditions for B–branes [75], which read Im(eiθeB+FeiJ), are mapped by mirror symmetry to the stability conditions for A–branes, Im(eiθeFΩ). A similar mapping was argued in [76] for the expression of the central charge for B–branes, R B e B+iJch(E) q Td(M) Td(B) and for A–”
- Exact solutions for supersymmetric stationary black hole composites (2003, unknown): “We also give an example of moduli-dependent black hole entropy.”