Abstract

We develop a stochastic analysis of the sine-Gordon Euclidean quantum field (cos⁡(βφ))2(\cos (βφ))_2 on the full space up to the second threshold, i.e. for β2<6πβ^2 < 6 π. The basis of our method is a forward-backward stochastic differential equation (FBSDE) for a decomposition (Xt)t⩾0(X_t)_{t \geqslant 0} of the interacting Euclidean field X∞X_{\infty} along a scale parameter t⩾0t \geqslant 0. This FBSDE describes the optimiser of the stochastic control representation of the Euclidean QFT introduced by Barashkov and one of the authors. We show that the FBSDE provides a description of the interacting field without cut-offs and that it can be used effectively to study the sine-Gordon measure to obtain results about large deviations, integrability, decay of correlations for local observables, singularity with respect to the free field, Osterwalder-Schrader axioms and other properties.

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