Two-dimensional delta-Bose gas: skew-product relative motions
Yu-Ting Chen
TL;DR
This work develops a stochastic path integral for the two-dimensional delta-Bose gas by deriving a non-exponential Feynman–Kac-type formula for the relative motion. The radial component is realized as BES$(0,β\downarrow)$ and the full relative motion as a complex skew-product diffusion, with an angular clock driven by circular Brownian motion. Two complementary proofs are provided: an excursion-based method and a lower-dimensional, SDE-based approach using BES$(-α,β\downarrow)$ and Macdonald-function drift ratios, which together establish strong well-posedness and a precise irregular drift structure. The results illuminate the non-Gaussian nature of the 2D delta interaction and connect to moments and critical phenomena in the two-dimensional stochastic heat equation, while also introducing a tractable lower-dimensional approximation framework that could extend to many-body settings.
Abstract
We prove a Feynman-Kac-type formula for the relative motion of the two-body delta-Bose gas in two dimensions. The multiplicative functional is not exponential, and the process is a skew-product diffusion uniquely extended in law, in the sense of Erickson [30], from ${\rm BES}(0,β{\downarrow})$ of Donati-Martin and Yor [27] as the radial part. We give two different proofs of the formula. The first uses the original excursion characterization of ${\rm BES}(0,β\downarrow)$, and the second is via the lower-dimensional Bessel processes at the expectation level. The latter proof contrasts the long-standing approach for delta-function interactions by adding mollifiers to the Laplacians since the present approximations are from "lower, fractional dimensions." Moreover, the second proof conducts a new study of ${\rm BES}(0,β\downarrow)$ as an SDE since we handle the drift via certain ratios of the Macdonald functions. The properties proven include the strong well-posedness and comparison of the SDE of ${\rm BES}(0,β\downarrow)$ for all initial conditions. In particular, this well-posedness contrasts the fact that the skew-product diffusion for the Feynman-Kac-type formula has a singular drift of $L^p_{\rm\tiny loc}$-integrability only for $ p\leq 2$.
