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On the Landau-Ginzburg description of Boundary CFTs and special Lagrangian submanifolds
High Energy Physics - Theory · Submitted 27 Mar 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find that the boundary conditions must necessarily have vanishing Poisson bracket with the combination (W(\phi)-\bar{W}(\bar{\phi})), where W(\phi) is the appropriate superpotential for the hypersurface.
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The abstract, sentence by sentence
We consider Landau-Ginzburg (LG) models with boundary conditions preserving A-type N=2 supersymmetry. We show the equivalence of a linear class of boundary conditions in the LG model to a particular class of boundary states in the corresponding CFT by an explicit computation of the open-string Witten index in the LG model. We extend the linear class of boundary conditions to general non-linear boundary conditions and determine their consistency with A-type N=2 supersymmetry. This enables us to provide a microscopic description of special Lagrangian submanifolds in C^n due to Harvey and Lawson. We generalise this construction to the case of hypersurfaces in P^n. We find that the boundary conditions must necessarily have vanishing Poisson bracket with the combination (W(\phi)-\bar{W}(\bar{\phi})), where W(\phi) is the appropriate superpotential for the hypersurface. An interesting application considered is the T^3 supersymmetric cycle of the quintic in the large complex structure limit.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider Landau-Ginzburg (LG) models with boundary conditions preserving A-type N=2 supersymmetry. | background 0.71 | 0.61 | 0.04 | asserted 0.80 |
| s1 | We show the equivalence of a linear class of boundary conditions in the LG model to a particular class of boundary states in the corresponding CFT by an explicit computation of the open-string Witten index in the LG model. | result 0.81 | 0.96 | 0.32 | asserted 1.00 |
| s2 | We extend the linear class of boundary conditions to general non-linear boundary conditions and determine their consistency with A-type N=2 supersymmetry. | contribution 0.97 | 0.96 | 0.11 | asserted 0.99 |
| s3 | This enables us to provide a microscopic description of special Lagrangian submanifolds in C^n due to Harvey and Lawson. | result 0.42 | 0.85 | 0.31 | asserted 0.99 |
| s4 | We generalise this construction to the case of hypersurfaces in P^n. | contribution 0.99 | 0.90 | 0.07 | asserted 0.99 |
| s5 | We find that the boundary conditions must necessarily have vanishing Poisson bracket with the combination (W(\phi)-\bar{W}(\bar{\phi})), where W(\phi) is the appropriate superpotential for the hypersurface. | result 1.00 | 0.93 | 0.32 | asserted 1.00 |
| s6 | An interesting application considered is the T^3 supersymmetric cycle of the quintic in the large complex structure limit. | contribution 0.86 | 0.76 | 0.05 | asserted 0.92 |
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Original abstract
We consider Landau-Ginzburg (LG) models with boundary conditions preserving A-type N=2 supersymmetry. We show the equivalence of a linear class of boundary conditions in the LG model to a particular class of boundary states in the corresponding CFT by an explicit computation of the open-string Witten index in the LG model. We extend the linear class of boundary conditions to general non-linear boundary conditions and determine their consistency with A-type N=2 supersymmetry. This enables us to provide a microscopic description of special Lagrangian submanifolds in C^n due to Harvey and Lawson. We generalise this construction to the case of hypersurfaces in P^n. We find that the boundary conditions must necessarily have vanishing Poisson bracket with the combination (W(\phi)-\bar{W}(\bar{\phi})), where W(\phi) is the appropriate superpotential for the hypersurface. An interesting application considered is the T^3 supersymmetric cycle of the quintic in the large complex structure limit.
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