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首页> 外文期刊>The European physical journal, B. Condensed matter physics >Limited coagulation-diffusion dynamics in inflating spaces
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Limited coagulation-diffusion dynamics in inflating spaces

机译:有限的凝血 - 扩散动态在充气空间中

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We consider the one-dimensional coagulation-diffusion problem on a dynamical expanding linear lattice, in which the effect of the coagulation process is balanced by the dilatation of the distance between particles. Distances x(t) follow the general law x(t)/x(t)=alpha (1+alpha t/beta)(-1) with growth rate alpha and exponent beta, describing both algebraic and exponential (beta = infinity) growths. In the space continuous limit, the particle dynamics is known to be subdiffusive, with the diffusive length varying like t(1/2-beta) for beta < 1/2, logarithmic for = 1/2, and reaching a finite value for all beta > 1/2. We interpret and characterize quantitatively this phenomenon as a second order phase transition between an absorbing state and a localized state where particles are not reactive. We furthermore investigate the case when space is discrete and use a generating function method to solve the time differential equation associated with the survival probability. This model is then compared with models of growth on geometrically constrained two-dimensional domains, and with the theory of fractional diffusion in the subdiffusive case. We found in particular a duality relation between the diffusive lengths in the inflating space and the fractional theory.
机译:我们考虑一种动态膨胀线性晶格上的一维凝固 - 扩散问题,其中通过颗粒之间的距离扩张来平衡凝固过程的效果。距离X(t)遵循一般法律x(t)/ x(t)=α(1 +αt / beta)( - 1),生长速率α和指数β,描述代数和指数(beta =无穷大)生长。在空间连续极限中,已知粒子动力学是副屈光度的,其衍射长度与β<1/2的t(1/2-β)变化,对数为 = 1/2,并达到有限所有beta> 1/2的价值。我们将该现象定量地解释和表征,作为吸收状态和颗粒不反应的局部状态之间的二阶相转变。我们进一步调查空间是离散的情况并使用产生功能方法来解决与生存概率相关的时间微分方程。然后将该模型与几何限制二维域的生长模型进行比较,以及沉贴案中的分数扩散理论。我们特别发现膨胀空间中的漫射长度与分数理论之间的二元关系。

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