Beta Ensembles, Quantum Painleve Equations and Isomonodromy Systems

This is a review of recent developments in the theory of beta ensembles of random matrices and their relations with conformal filed theory (CFT). There are (almost) no new results here. equations of Belavin-Polyakov-Zamolodchikov (BPZ) type occupy the main stage. This article can serve as a guide on appearances and studies of quantum Painleve and more general multidimensional linear equations of Belavin-Polyakov-Zamolodchikov (BPZ) type in literature. We demonstrate how BPZ equations of CFT arise from beta-ensemble eigenvalue integrals. Quantum Painleve equations are relatively simple instances of BPZ or confluent BPZ equations, they are PDEs in two independent variables ("time" and "space"). While CFT is known as quantum integrable theory, here we focus on the appearing links of beta-ensembles and CFT with classical integrable structure and isomonodromy systems. The central point is to show on the example of quantum Painleve II (QPII) [94] how classical integrable structure can be extended to general values of beta (or CFT central charge c), beyond the special cases beta = 2 (c = 1) and c -> infinity where its appearance is well -established. We also discuss an a priori very different important approach, the ODE/IM correspondence giving information about complex quantum integrable models, e.g. CFT, from some stationary Schrodinger ODEs. Solution of the ODEs depends on (discrete) symmetries leading to functional equations for Stokes multipliers equivalent to discrete integrable Hirota-type equations. The separation of "time" and "space" variables, a consequence of our integrable structure, also leads to Schrodinger ODEs and thus may have a connection with ODE/IM methods.