Boundary Rings and N=2 Coset Models
arXiv:hep-th/0011107 · doi:10.1016/S0550-3213(02)00019-6
Abstract
We investigate boundary states of N=2 coset models based on Grassmannians Gr(n,n+k), and find that the underlying intersection geometry is given by the fusion ring of U(n). This is isomorphic to the quantum cohomology ring of Gr(n,n+k+1), and thus can be encoded in a ``boundary'' superpotential whose critical points correspond to the boundary states. In this way the intersection properties can be represented in terms of a soliton graph that forms a generalized, Z_{n+k+1} symmetric McKay quiver. We investigate the spectrum of bound states and find that the rational boundary CFT produces only a small subset of the possible quiver representations.
40p, 5 figs, refs added, typos and minor errors corrected
References in corpus (1)
Cited by in corpus (12)
- Magnetic Monopole Dynamics, Supersymmetry, and Duality
- K-Theory from a physical perspective
- Organizing boundary RG flows
- Fusion of symmetric -branes and Verlinde rings
- A new kind of McKay correspondence from non-Abelian gauge theories
- D-branes in N=2 coset models and twisted equivariant K-theory
- K-theoretical boundary rings in N=2 coset models
- BRST construction of D-branes in SU(2) WZW model
- Comments on D-branes in Kazama-Suzuki models and Landau-Ginzburg theories
- Twisted boundary states in Kazama-Suzuki models
- D-branes and matrix factorisations in supersymmetric coset models
- Supersymmetric WZW models and twisted K-theory of SO(3)