On the equilibrium measure for the Lukyanov integral
Charlie Dworaczek Guera, Karol K. Kozlowski
TL;DR
The paper rigorously constructs the $N$-dependent equilibrium measure governing the leading large-$N$ behavior of Lukyanov's integral ratio, providing a precise variational framework and an explicit Wiener-Hopf–Riemann–Hilbert representation for the equilibrium density. It proves the measure is Lebesgue continuous with a square-root vanishing density on a single interval, and derives explicit large-$N$ expansions for the endpoints. Using these results, it obtains the leading large-$N asymptotics of the interpolating integral, showing the Lukyanov ratio behaves as $(N/\mathfrak{r})^{\alpha^2/2}$ times a field-expectation factor, with a remainder that is presently bounded by $O(\sqrt{N}\,\tau_N^2)$ and conjectured to reduce to $O(1)$ via loop equations. Overall, the work provides a solid rigorous foundation for the conjectured large-$N structure and paves the way for a complete asymptotic expansion through analytic techniques.
Abstract
In 2000, Lukyanov conjectured that a certain ratio of $N$-fold integrals should provide access, in the large-$N$ regime, to the ground state expectation value of the exponential of the Sinh-Gordon quantum field in 1+1 dimensions and finite volume $R$. This work aims at rigorously constructing the fundamental objects necessary to address the large-$N$ analysis of such integrals. More precisely, we construct and establish the main properties of the the equilibrium measure minimising a certain $N$-dependent energy functional that naturally arises in the study of the leading large-$N$ behaviour of the Lukyanov integral. Our construction allows us to heuristically advocate the leading term in the large-$N$ asymptotic behaviour of the mentioned ratio of Lukyanov integrals, hence supporting Lukyanov's prediction -- obtained by other means -- on the exponent $σ$ of the power-law $N^σ$ term of its asymptotic expansion as $N\rightarrow + \infty$.
