Current Fluctuations for the Boundary-Driven Zero-Range Process on Graphs: Microscopic Versus Macroscopic Approach and a Theory of Non-reversible Resistor-Like Networks
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引用次数: 0
Abstract
We compute the joint large deviation rate functional in the limit of large time for the current flowing through the edges of a finite graph on which a boundary-driven system of stochastic particles evolves with zero-range dynamics. This generalizes one-dimensional results previously obtained with different approaches (Bertini et al. in J Stat Phys 123(2):237–276, 2006; Harris et al. in J Stat Mech Theory Exp 2005:P08003, 2005); our alternative techniques illuminate various connections and complementary perspectives. In particular, we here use a variational approach to derive the rate functional by contraction from a level 2.5 large deviation rate functional. We perform an exact minimization and finally obtain the rate functional as a variational problem involving a superposition of cost functions for each edge. The contributions from different edges are not independent since they are related by the values of a potential function on the nodes of the graph. The rate functional on the graph is a microscopic version of the continuous rate functional predicted by the macroscopic fluctuation theory (Bertini et al. in Rev Mod Phys 87(2):593–636, 2015), and we indeed show a convergence in the scaling limit. If we split the graph into two connected regions by a cutset and are interested just in the current flowing through the cutset, we find that the result is the same as that of an effective system composed of only one effective edge [as happens at macroscopic level and is expected also for other models (Akkermans et al. in Europhys Lett 103(2):20001, 2013)]. The characteristics of this effective edge are related to the “capacities” of the graph and can be obtained by a reduction using elementary transformations as in electrical networks; specifically, we treat components in parallel, in series, and in N-star configurations (reduced to effective complete N-graphs). Our reduction procedure is directly related to the reduction to the trace process (Landim in Probab Surv 16:143–227, 2019) and, since the dynamics is in general not reversible, it is also closely connected to the theory of non-reversible electrical networks in Balázs and Folly (Am Math Mon 123(7):657–682, 2016).
本文计算了随机粒子边界驱动系统以零范围动力学演化的有限图边缘电流在大时间极限下的联合大偏差率泛函。这概括了以前用不同方法得到的一维结果(Bertini et al. in J Stat Phys 123(2): 237-276, 2006;Harris et al. J Stat Mech Theory Exp 2005:P08003, 2005);我们的替代技术阐明了各种联系和互补的观点。特别地,我们在这里使用变分方法从2.5级大偏差率函数中通过收缩推导出速率函数。我们执行一个精确的最小化,并最终获得速率函数作为一个涉及每条边的成本函数的叠加的变分问题。来自不同边的贡献不是独立的,因为它们是由图节点上的势能函数的值联系起来的。图上的速率泛函是宏观涨落理论预测的连续速率泛函的微观版本(Bertini et al. in Rev Mod Phys 87(2): 593-636, 2015),我们确实在尺度极限上显示出收敛性。如果我们通过割集将图分割成两个相连的区域,并且只对流经割集的电流感兴趣,我们发现结果与仅由一条有效边组成的有效系统的结果相同[这发生在宏观层面,也适用于其他模型(Akkermans et al. in Europhys Lett 103(2): 2001,2013)]。这种有效边的特征与图的“容量”有关,可以通过使用电气网络中的初等变换进行约简来获得;具体来说,我们以并行、串联和n星结构(简化为有效的完全n图)来处理组件。我们的还原过程与还原到跟踪过程直接相关(Landim in Probab Surv 16:143-227, 2019),并且,由于动力学通常是不可逆的,它也与Balázs和Folly中的不可逆电网络理论密切相关(Am Math Mon 123(7): 657-682, 2016)。
期刊介绍:
The two journals Annales de l''Institut Henri Poincaré, physique théorique and Helvetica Physical Acta merged into a single new journal under the name Annales Henri Poincaré - A Journal of Theoretical and Mathematical Physics edited jointly by the Institut Henri Poincaré and by the Swiss Physical Society.
The goal of the journal is to serve the international scientific community in theoretical and mathematical physics by collecting and publishing original research papers meeting the highest professional standards in the field. The emphasis will be on analytical theoretical and mathematical physics in a broad sense.