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Super Liouville Theory with Boundary

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arxiv hep-th/0202032 v3 pith:7ZGAVFRF submitted 2002-02-06 hep-th

classification hep-th
keywords boundaryfunctionssomestatesdegenerateliouvillemodularobtained
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We study N=1 super Liouville theory on worldsheets with and without boundary. Some basic correlation functions on a sphere or a disc are obtained using the properties of degenerate representations of superconformal algebra. Boundary states are classified by using the modular transformation property of annulus partition functions, but there are some of those whose wave functions cannot be obtained from the analysis of modular property. There are two ways of putting boundary condition on supercurrent, and it turns out that the two choices lead to different boundary states in quality. Some properties of boundary vertex operators are also presented. The boundary degenerate operators are shown to connect two boundary states in a way slightly complicated than the bosonic case.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Towards the super Virasoro minimal string

    hep-th 2025-05 conditional novelty 7.0 of 10

    The authors derive the timelike super Liouville structure constants from crossing symmetry and construct a tentative Type 0A/0B super Virasoro minimal string whose sphere three-point functions vanish only after sign c...

  2. Instanton-Induced Closed-String Amplitudes in Minimal Superstring Theory at Subleading Order

    hep-th 2026-06 unverdicted novelty 6.0 of 10

    Explicit computation of instanton-induced amplitudes in minimal superstring theories at subleading order, after regulating open-string degenerations with string field theory, yields exact agreement with DDK-KPZ scaling.

  3. Further aspects of Supersymmetric Virasoro Minimal Strings

    hep-th 2025-06 conditional novelty 6.0 of 10

    The paper defines the 0B supersymmetric Virasoro minimal string as an average of two 0A models and shows its loop correlators beyond the leading disc and cylinder vanish to all orders in perturbation theory.

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