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Intermittence and nonlinear parabolic stochastic partial differential equations

  
@article{EJP614,
	author = {Mohammud Foondun and Davar Khoshnevisan},
	title = {Intermittence and nonlinear  parabolic stochastic partial differential equations},
	journal = {Electron. J. Probab.},
	fjournal = {Electronic Journal of Probability},
	volume = {14},
	year = {2009},
	keywords = {Stochastic partial differential equations, Levy processes},
	abstract = {We consider nonlinear parabolic 	SPDEs of the form  	$\partial_t u={\cal L} u + \sigma(u)\dot w$, where 	$\dot w$ denotes space-time white noise, 	$\sigma:R\to R$ is [globally] Lipschitz continuous, 	and $\cal L$ is the $L^2$-generator of a L'evy process. 	We present precise criteria for existence 	as well as uniqueness of solutions. 	More significantly, we prove that these solutions grow 	in time with at most a precise exponential rate.	 	We establish also that when $\sigma$ is globally Lipschitz 	and asymptotically sublinear, the solution 	to the nonlinear heat equation is ``weakly intermittent,'' 	provided that the symmetrization 	of $\cal L$ is recurrent and the initial data is sufficiently 	large. 	 	Among other things, 	our results lead to general 	formulas for the upper second-moment 	Liapounov exponent of the parabolic 	Anderson model for $\cal L$ in dimension $(1+1)$. When 	${\cal L}=\kappa\partial_{xx}$ for $\kappa>0$, these formulas  	agree with the earlier results of statistical physics 	(Kardar (1987), Krug and Spohn (1991), Lieb and Liniger (1963)), and also probability theory (Bertini and Cancrini (1995), Carmona and Molchanov (1994)) in the two exactly-solvable cases. That is  	when $u_0=\delta_0$ or $u_0\equiv 1$; in those cases 	the moments of the solution to the SPDE can be computed (Bertini and Cancrini (1995)).},
	pages = {no. 21, 548-568},
	issn = {1083-6489},
	doi = {10.1214/EJP.v14-614},    
        url = {http://ejp.ejpecp.org/article/view/614}}