Four-point correlation numbers in super Minimal Liouville Gravity in the Ramond sector
Vladimir Belavin, Juan Ramos Cabezas, Boris Runov

TL;DR
This paper derives a closed-form analytic expression for four-point correlation numbers in super Minimal Liouville Gravity's Ramond sector, extending previous work on three-point functions and utilizing higher equations of motion.
Contribution
It introduces a novel analytic method to compute four-point correlation numbers in the Ramond sector of super Minimal Liouville Gravity, building on prior three-point function evaluations.
Findings
Derived a closed-form expression for four-point correlation numbers.
Extended the higher equations of motion approach to the Ramond sector.
Connected four-point functions with boundary contributions from OPE structures.
Abstract
In this work, we continue the investigation of correlation numbers in super Minimal Liouville Gravity (SMLG), with physical fields in the Ramond sector. Building upon our previous construction of physical operators and the evaluation of three-point correlation functions involving Ramond and Neveu-Schwarz (NS) insertions, we now turn to the analytic computation of four-point correlation numbers. This development is motivated by the framework established for the bosonic Minimal Liouville Gravity and its supersymmetric NS analog, where the integration over moduli space in correlation functions can be performed explicitly using the higher equations of motion (HEM) in Liouville theory. In particular, if one of the insertions corresponds to a degenerate field, the four-point amplitude can be expressed in terms of boundary contributions obtained from the OPE structure of…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsBlack Holes and Theoretical Physics · Quantum and Classical Electrodynamics · Quantum Electrodynamics and Casimir Effect
