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We investigate fractional stochastic Navier-Stokes equations in d 3, driven by the random force (-) ^{2} which, as we show, corresponds to a fractional version of the Landau-Lifshitz random force in the physics literature. We obtain the existence and uniqueness of martingale solutions on the torus Tᵈ for > d2. For 1 the equation is supercritical and we regularize the problem by introducing a Galerkin approximation and we study the large scale behavior of the truncated model on ᵈ. We show that the nonlinear term in the Galerkin approximation vanishes on large scales when < 1 and the model converges to the linearized equation. For = 1 the nonlinear term gives a nontrivial contribution to the large scale beahvior, and we conjecture that the large scale behavior is given by a linear model with strictly larger effective diffusivity compared to simply dropping the nonlinear term. The effective diffusivity is explicitly given in terms of the model parameters.
Jin et al. (Thu,) studied this question.