Structure Constants in the $N=1$ Super-Liouville Field Theory

Details Structure Constants in the $N=1$ Super-Liouville Field Theory Structure Constants in the $N=1$ Super-Liouville Field Theory

1996-07-15

arxiv.org/abs/hep-th/9607120v1

Nucl.Phys. B496 (1997) 451-464

Physics

High Energy Physics

High Energy Physics - Theory

LaTeX file, 17 pages, no figures

Scientific paper

10.1016/S0550-3213(97)00218-6

The symmetry algebra of $N=1$ Super-Liouville field theory in two dimensions is the infinite dimensional $N=1$ superconformal algebra, which allows one to prove, that correlation functions, containing degenerated fields obey some partial linear differential equations. In the special case of four point function, including a primary field degenerated at the first level, this differential equations can be solved via hypergeometric functions. Taking into account mutual locality properties of fields and investigating s- and t- channel singularities we obtain some functional relations for three- point correlation functions. Solving this functional equations we obtain three-point functions in both Neveu-Schwarz and Ramond sectors.

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