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arXiv 2005.11969cond-mat.stat-mech
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传播到不稳定状态的随机反应锋的速度涨落:强推锋

Velocity fluctuations of stochastic reaction fronts propagating into an unstable state: strongly pushed fronts

Evgeniy Khain, Baruch Meerson, Pavel Sasorov

摘要:

由于反应和扩散的散粒噪声,传播到不稳定状态的反应扩散波前的经验速度会发生波动。在一定条件下,这些波动可以描述为参考系中以波前的平均速度运动的扩散过程。在这里,我们解决了推前,在确定性限制的前端速度的影响,高阶反应,因此大于线性传播速度。对于一个子类的这些前线-强推前线-的有效扩散常数$D_f\sim 1/N$的前线可以计算,在领先的顺序,通过微扰理论在$1/N \ll 1$,其中$N\gg 1$是典型的粒子数在过渡区。然而,这种微扰理论高估了前沿的一些快速粒子的贡献。我们建议一个更一致的计算,通过引入一个空间积分截止在一个距离,超过该平均粒子数是1阶。这导致对$D_f$的非微扰修正,其甚至在接近强推锋和弱推锋之间的过渡点处成为主导。在过渡点处,我们得到对$D_f$的$1/N$缩放的对数校正。我们还发现了另一个相当令人惊讶的,在前沿的快速粒子的影响。由于这些粒子,波前的位置波动可以被描述为仅在具有持续时间$Δt \gg τ_N$的非常长的时间间隔上的扩散过程,其中$τ_N$标度为$N$。在中间时刻,锋的位置波动非常大,而且不扩散。我们广泛的蒙特卡罗模拟的一个特定的反应晶格气模型支持这些结论。

英文摘要:

The empirical velocity of a reaction-diffusion front, propagating into an unstable state, fluctuates because of the shot noises of the reactions and diffusion. Under certain conditions these fluctuations can be described as a diffusion process in the reference frame moving with the average velocity of the front. Here we address pushed fronts, where the front velocity in the deterministic limit is affected by higher-order reactions and is therefore larger than the linear spread velocity. For a subclass of these fronts -- strongly pushed fronts -- the effective diffusion constant $D_f\sim 1/N$ of the front can be calculated, in the leading order, via a perturbation theory in $1/N \ll 1$, where $N\gg 1$ is the typical number of particles in the transition region. This perturbation theory, however, overestimates the contribution of a few fast particles in the leading edge of the front. We suggest a more consistent calculation by introducing a spatial integration cutoff at a distance beyond which the average number of particles is of order 1. This leads to a non-perturbative correction to $D_f$ which even becomes dominant close to the transition point between the strongly and weakly pushed fronts. At the transition point we obtain a logarithmic correction to the $1/N$ scaling of $D_f$. We also uncover another, and quite surprising, effect of the fast particles in the leading edge of the front. Because of these particles, the position fluctuations of the front can be described as a diffusion process only on very long time intervals with a duration $Δt \gg τ_N$, where $τ_N$ scales as $N$. At intermediate times the position fluctuations of the front are anomalously large and non-diffusive. Our extensive Monte-Carlo simulations of a particular reacting lattice gas model support these conclusions.

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