首页> 外文会议>NATO Advanced Research Workshop on Continuum Models and Discrete Systems; 20030630-0704; Shoresh(IL) >VARIABLE RANGE HOPPING CONDUCTION IN COMPLEX SYSTEMS AND A PERCOLATION MODEL WITH TUNNELING
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VARIABLE RANGE HOPPING CONDUCTION IN COMPLEX SYSTEMS AND A PERCOLATION MODEL WITH TUNNELING

机译:复杂系统中的变径跳变传导和带隧道的渗透模型

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For the low-temperature electrical conductance of a disordered quantum insulator in d-dimensions, Mott had proposed his Variable Range Hopping (VRH) formula, G(T) = Go exp[- (T_0/T)~γ], where G_0 is a material constant and T_0 is a characteristic temperature scale. For disordered but non-interacting carrier charges, Mott had found that γ = 1/(d + 1) in d dimensions. Later on, Efros and Shkolvskii found that for a pure (i.e., disorder-free) quantum insulator with interacting charges, γ = 1/2, independent of d. Recent experiments indicate that γ is either (ⅰ) larger than any of the above predictions; and, (ⅱ) more intriguingly, it seems to be a function of p, the dopant concentration. We investigate this issue with a semi-classical or semi-quantum RRTN (Random Resistor cum Tunneling-bond Network) model, developed by us in the 1990's. These macroscopic granular/percolative composites are built up from randomly placed meso- or nanoscopic coarse-grained clusters, with two pbe-nomenological functions for the temperature-dependence of the metallic and the semi-conducting bonds. We find that our RRTN model (in 2D, for simplicity) also captures this continuous change of γ with p, satisfactorily.
机译:对于d维无序量子绝缘子的低温电导,Mott提出了他的可变跳频(VRH)公式,G(T)= Go exp [-(T_0 / T)〜γ],其中G_0为材料常数,T_0是特征温度标度。对于无序但不相互作用的载流子电荷,Mott发现在d维度上γ= 1 /(d +1)。后来,Efros和Shkolvskii发现对于具有相互作用电荷的纯(即无序)量子绝缘子,γ= 1/2,与d无关。最近的实验表明,γ比上述任何一个预测值都大(?);更有趣的是,它似乎是掺杂剂浓度p的函数。我们使用由我们在1990年代开发的半经典或半量子RRTN(随机电阻器和隧穿键合网络)模型来研究此问题。这些宏观的颗粒/渗流复合材料是由随机放置的中观或纳米级粗粒团簇构成的,具有金属和半导体键随温度变化的两种贝贝命名学功能。我们发现,我们的RRTN模型(为简单起见,在2D模式下)也令人满意地捕获了γ与p的连续变化。

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