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Non-Gaussian Resistance Fluctuations in Disordered Materials

机译:无序材料中的非高斯电阻波动

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We study the distribution of resistance fluctuations of conducting thin films with different levels of internal disorder. The film is modeled as a resistor network in a steady state determined by the competition between two biased processes, breaking and recovery of the elementary resistors. The fluctuations of the film resistance are calculated by Monte Carlo simulations which are performed under different bias conditions, from the linear regime up to the threshold for electrical breakdown. Depending on the value of the external current, on the level of disorder and on the size of the system, the distribution of the resistance fluctuations can exhibit significant deviations from Gaussianity. As a general trend, a size dependent, non universal distribution is found for systems with low and intermediate disorder. However, for strongly disordered systems, close to the critical point of the conductor-insulator transition, the non-Gaussianity persists when the size is increased and the distribution of resistance fluctuations is well described by the universal Bramwell-Holdsworth-Pinton distribution.
机译:我们研究了不同含量的内部病症进行薄膜的电阻波动的分布。该薄膜以稳定状态为电阻网络建模,其由两个偏置过程之间的竞争确定,断裂和恢复基本电阻器之间的竞争。通过在不同偏置条件下执行的蒙特卡罗模拟来计算膜电阻的波动,从线性制度从直到电击穿的阈值进行。根据外部电流的值,在疾病程度和系统的大小上,电阻波动的分布可以表现出与高斯的显着偏差。作为一般趋势,尺寸依赖性,非普遍分布用于低和中间疾病的系统。然而,对于强烈无序的系统,接近导体绝缘体过渡的临界点,当尺寸增加并且通过通用Bramwell-Holdsworth-Cinton分布很好地描述了抗性波动的分布的非高斯度仍然存在。

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