Exact solutions by integrals of the non-stationary elliptic Calogero-Sutherland equation
arXiv:1908.00529 · doi:10.1093/integr/xyaa001
Abstract
We use generalized kernel functions to construct explicit solutions by integrals of the non-stationary Schrödinger equation for the Hamiltonian of the elliptic Calogero-Sutherland model (also known as elliptic Knizhnik-Zamolodchikov-Bernard equation). Our solutions provide integral represenations of elliptic generalizations of the Jack polyomials.
arXiv comment26 pages
References in corpus (12)
- Excited States of Calogero-Sutherland Model and Singular Vectors of the Algebra
- Differential equation for four-point correlation function in Liouville field theory and elliptic four-point conformal blocks
- Explicit solution of the (quantum) elliptic Calogero-Sutherland model
- Remarkable identities related to the (quantum) elliptic Calogero-Sutherland model
- Source identity and kernel functions for elliptic Calogero-Sutherland type systems
- Deformed Calogero-Sutherland model and fractional Quantum Hall effect
- Unitarity of the Knizhnik-Zamolodchikov-Bernard connection and the Bethe Ansatz for the elliptic Hitchin systems
- Orthogonality of super-Jack polynomials and a Hilbert space interpretation of deformed Calogero-Moser-Sutherland operators
- Source identity and kernel functions for Inozemtsev-type systems
- Quantum integrability of the deformed elliptic Calogero-Moser problem
- Bosonization and integral representation of solutions of the Knizhnik-Zamolodchikov-Bernard equations
- Special functions, conformal blocks, Bethe ansatz, and SL(3,Z)