2008
DOI: 10.1063/1.2982234
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Poisson sigma model with branes and hyperelliptic Riemann surfaces

Abstract: The relevant superpropagators for n branes are defined as gauge fixed homotopy operators of a complex of differential forms on n sided polygons Pn with particular "alternating" boundary conditions. In presence of more than three branes we use first order Riemann theta functions with odd singular characteristics on the Jacobian variety of a hyperelliptic Riemann surface (canonical setting). In genus g the superpropagators present g zero modes contributions.

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Cited by 6 publications
(7 citation statements)
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“…We finally observe that all previous formulae are special cases of the main result in [9], where general (super)propagators for the Poisson σ-model in the presence of n branes, n ≥ 1, are explicitly produced.…”
Section: 32mentioning
confidence: 71%
“…We finally observe that all previous formulae are special cases of the main result in [9], where general (super)propagators for the Poisson σ-model in the presence of n branes, n ≥ 1, are explicitly produced.…”
Section: 32mentioning
confidence: 71%
“…Even though not justified in terms of the BV formalism, this choice of propagator was done before in [2] for Chern-Simons theory out of purely topological reasons, and later extended to BF theories in [7]. A propagator with these properties also appears in [13] for the Poisson sigma model on the interior of a polygon.…”
Section: Bv Formalism and Zero Modesmentioning
confidence: 99%
“…The differential forms are obtained from the propagator ω, see (14), and the form φ, see (13). Let Γ ∈ G (k1,...,kn),m .…”
Section: Weightsmentioning
confidence: 99%
“…We have an explicit propagator for the PSM, i.e. using the superfields of it, on a disk with alternating boundary conditions, which was computed in [14], in [26] and, in full generality, in [31]. C.1.…”
Section: Appendix C On the Propagatormentioning
confidence: 99%