Physical review. E · 2018 · 25 citations · 51 references
Natural SciencesMathematicsPhysicsCondensed Matter PhysicsProbability TheoryStochastic ProcessesDissipative SystemsInterface PhysicsSecond Law Of ThermodynamicsStatistical MechanicsStochastic Differential EquationsFluctuation RelationsFluctuation TheoremsFluctuation TheoryNeumann Boundary Conditions
Consider a stochastic interface $h(x,t)$, described by the $1+1$ Kardar-Parisi-Zhang (KPZ) equation on the half line $x\ensuremath{\ge}0$. The interface is initially flat, $h(x,t=0)=0$, and driven by a Neumann boundary condition ${\ensuremath{\partial}}_{x}h(x=0,t)=A$ and by the noise. We study the short-time probability distribution $\mathcal{P}\left(H,A,t\right)$ of the one-point height $H=h(x=0,t)$. Using the optimal fluctuation method, we show that $\ensuremath{-}ln\mathcal{P}\left(H,A,t\right)$ scales as ${t}^{\ensuremath{-}1/2}s\left(H,A{t}^{1/2}\right)$. For small and moderate $|A|$ this more general scaling reduces to the familiar simple scaling $\ensuremath{-}ln\mathcal{P}\left(H,A,t\right)\ensuremath{\simeq}{t}^{\ensuremath{-}1/2}s(H)$, where $s$ is independent of $A$ and time and equal to one half of the corresponding large-deviation function for the full-line problem. For large $|A|$ we uncover two asymptotic regimes. At very short time the simple scaling is restored, whereas at intermediate times the scaling remains more general and $A$-dependent. The distribution tails, however, always exhibit the simple scaling in the leading order.
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