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The depinning transition critical point is manifested as power-law distributed avalanches exhibited by slowly driven elastic interfaces in quenched random media. Here we show that since avalanches with different starting heights relative to the mean interface height or different initial local interface curvatures experience different excess driving forces due to elasticity, avalanches close to the “global” critical point of non-mean field systems can be separated into populations of subcritical, critical and supercritical ones. The asymmetric interface height distribution results in an excess of supercritical avalanches, manifested as a “bump” in the avalanche size distribution cutoff.

生成讲解博客的中文版本

生成AI智能校验的中文版本