Abstract

We study the two-dimensional stochastic nonlinear wave equation (SNLW) and stochastic nonlinear heat equation (SNLH) with a quadratic nonlinearity, forced by a fractional derivative (of order $\alpha > 0$) of a space-time white noise. In particular, we show that the well-posedness theory breaks at $\alpha = \frac 12$ for SNLW and at $\alpha = 1$ for SNLH. This provides a first example showing that SNLW behaves less favorably than SNLH. (i) As for SNLW, Deya (2020) essentially proved its local well-posedness for $0 < \alpha < \frac 12$. We first revisit this argument and establish multilinear smoothing of order $\frac 14$ on the second order stochastic term in the spirit of a recent work by Gubinelli, Koch, and Oh (2018). This allows us to simplify the local well-posedness argument for some range of $\alpha $. On the other hand, when $\alpha \geq \frac 12$, we show that SNLW is ill-posed in the sense that the second order stochastic term is not a continuous function of time with values in spatial distributions. This shows that a standard method such as the Da Prato-Debussche trick or its variant, based on a higher order expansion, breaks down for $\alpha \ge \frac 12$. (ii) As for SNLH, we establish analogous results with a threshold given by $\alpha = 1$. These examples show that in the case of rough noises, the existing well-posedness theory for singular stochastic PDEs breaks down before reaching the critical values ($\alpha = \frac 34$ in the wave case and $\alpha = 2$ in the heat case) predicted by the scaling analysis (due to Deng, Nahmod, and Yue (2019) in the wave case and due to Hairer (2014) in the heat case).

Highlights

  • 1.1 Singular stochastic PDEsIn this paper, we study the following stochastic nonlinear wave equation (SNLW) on T2 = (R/2πZ)2:∂t2u + (1 − ∆)u + u2 = ∇ αξ (u, ∂tu)|t=0 = (u0, u1)(x, t) ∈ T2 × R+, and the stochastic nonlinear heat equation (SNLH) on T2: (1.1)∂tu + (1 − ∆)u + u2 = ∇ αξ u|t=0 = u0(x, t) ∈ T2 × R+, (1.2)√ where ∇ = 1 − ∆ and α > 0

  • We study the following stochastic nonlinear wave equation (SNLW) on T2 = (R/2πZ)2:

  • Both equations are endowed with a quadratic nonlinearity and forced by an α-derivative of a (Gaussian) space-time white noise ξ on T2 × R+

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Summary

Singular stochastic PDEs

It was essential to exploit multilinear smoothing in the construction of stochastic objects and to introduce paracontrolled operators While this comparison on the hyperbolic and parabolic Φ33-model shows that it may require more effort to study SNLW than SNLH, the resulting outcomes (local well-posedness on T3 with a quadratic nonlinearity forced by a space-time white noise) are essentially the same. Our main goal in this paper is to study to what extent the existing solution theory extends to handle rough noises in the context of SNLW and SNLH. For this purpose, we consider the simplest kind of nonlinearity (i.e. the quadratic nonlinearity) in (1.1) and (1.2). See Remark 1.13 for the case of fractional-in-time (and general fractional) noises

Stochastic nonlinear wave equation
Note that the extra smoothing is at most
Hs diverges for any
Stochastic nonlinear heat equation
Basic lemmas
Besov spaces and paraproduct estimates
Product estimates and discrete convolutions
Linear estimates
Tools from stochastic analysis
Stochastic nonlinear wave equation with rough noise
On the construction of the relevant stochastic objects
Divergence of the stochastic terms
Stochastic nonlinear heat equation with rough noise
Reformulation of SNLH
Full Text
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