Construction of a non-Gaussian and rotation-invariant $Φ^4$-measure and associated flow on ${\mathbb R}^3$ through stochastic quantization
Sergio Albeverio, Seiichiro Kusuoka
TL;DR
This work delivers a rigorous construction of a non‑Gaussian, rotation‑invariant, reflection‑positive probability measure $\mu$ associated with the $\varphi^4_3$ model by a stochastic quantization framework. Starting from regularized Gibbs measures $\mu_{M,N}$ with spatial and momentum cutoffs, the authors analyze the corresponding stochastic quantization equations to obtain tightness and weak convergence in weighted Besov spaces, yielding a limiting stationary flow $X$ whose invariant measure is $\mu$. They establish rotation/reflection invariance and reflection positivity of the limit, and prove that $\mu$ has compact Besov support and is non‑Gaussian, signaling a robust construction of Euclidean (and via OS/RS program, Minkowski) correlators for the $\varphi^4_3$ theory. The methodology hinges on a careful blend of Besov space techniques, paracontrolled calculus, and renormalization through Wick powers of an infinite‑dimensional Ornstein–Uhlenbeck process, enabling progress beyond torus‑based approaches to the full space ${\mathbb R}^3$. The results provide a solid probabilistic and analytic foundation for a stochastic quantization flow whose invariant measure captures essential non‑Gaussian and Euclidean‑invariant features of the $\varphi^4_3$ quantum field theory, with potential implications for understanding relativistic fields via Euclidean methods.
Abstract
A new construction of non-Gaussian, rotation-invariant and reflection positive probability measures $μ$ associated with the $\varphi ^4_3$-model of quantum field theory is presented. Our construction uses a combination of semigroup methods, and methods of stochastic partial differential equations (SPDEs) for finding solutions and stationary measures of the natural stochastic quantization associated with the $\varphi ^4_3$-model. Our starting point is a suitable approximation $μ_{M,N}$ of the measure $μ$ we intend to construct. $μ_{M,N}$ is parametrized by an $M$-dependent space cut-off function $ρ_M: {\mathbb R}^3\rightarrow {\mathbb R}$ and an $N$-dependent momentum cut-off function $ψ_N: \widehat{\mathbb R}^3 \cong {\mathbb R}^3 \rightarrow {\mathbb R}$, that act on the interaction term (nonlinear term and counterterms). The corresponding family of stochastic quantization equations yields solutions $(X_t^{M,N}, t\geq 0)$ that have $μ_{M,N}$ as an invariant probability measure. By a combination of probabilistic and functional analytic methods for singular stochastic differential equations on negative-indices weighted Besov spaces (with rotation invariant weights) we prove the tightness of the family of continuous processes $(X_t^{M,N},t \geq 0)_{M,N}$. Limit points in the sense of convergence in law exist, when both $M$ and $N$ diverge to $+\infty$. The limit processes $(X_t; t\geq 0)$ are continuous on the intersection of suitable Besov spaces and any limit point $μ$ of the $μ_{M,N}$ is a stationary measure of $X$. $μ$ is shown to be a rotation-invariant and non-Gaussian probability measure and we provide results on its support. It is also proven that $μ$ satisfies a further important property belonging to the family of axioms for Euclidean quantum fields, it is namely reflection positive.
