论文标题

部分可观测时空混沌系统的无模型预测

Activated hopping transport in nematic conducting aerogel at low temperatures

论文作者

Tsebro, V. I., Nikolaev, E. G., Lugansky, L. B., Kutuzov, M. S., Khmel'nitskii, R. A., Tonkikh, A. A., Khar'kovskii, A. I.

论文摘要

列内气凝胶的运输属性由高度定向的Al $ _2 $ o $ _3 \ cdot $ sio $ _2 $ nanofibers组成,含有大量缺陷的石墨烯壳。 9-40K范围内电阻率的温度依赖性严格遵循得出的公式来描述可变范围跳跃(VRH)电导率,当石墨烯壳中的层从4-6降低到4-6至1-2时,指数$α$从0.4 $变化为0.4。 $α$对壳厚度的依赖性可以通过同时变化跳传输的维度以及在费米水平附近局部状态密度的能量依赖性的特征来解释。 $α$以最小石墨烯壳厚度接近统一的事实表明,从VRH传输到最近的邻居跳跃(NNH)传输的逐渐过渡。在T = 4.2 K时测量的磁阻为负,随着石墨烯壳的厚度的减小而显着增加,并且通过较弱的定位情况近似,准确性较弱。相干长度与石墨烯晶粒尺寸的合理关系。研究中的导电气凝胶补充了在低温下表现出电子传输的众所周知的材料集,这是具有强载体定位的培养基的特征,也是负磁磁性的,通常在弱定位条件下表现出来。

The transport properties of nematic aerogels, which consist of highly oriented Al$_2$O$_3\cdot$SiO$_2$ nanofibers coated with a graphene shell with a large number of defects, are studied. The temperature dependences of the electrical resistivity in the range of 9-40K strictly follow the formula derived to describe the variable range hopping (VRH) conductivity, in which exponent $α$ changes from 0.4 to 0.9 when the number of layers in the graphene shell decreases from 4-6 to 1-2. The dependence of $α$ on the shell thickness can be explained by a simultaneous change in the dimensionality of hopping transport and the character of the energy dependence of the density of localized states near the Fermi level. The fact that $α$ approaches unity at the minimum graphene shell thickness indicates a gradual transition from VRH transport to nearest neighbor hopping (NNH) transport. The magnetoresistance measured at T = 4.2 K is negative, increases significantly with decreasing graphene shell thickness, and is approximated by a formula for the case of weak localization with a good accuracy. The phase coherence lengths are in a reasonable relation with the graphene grain sizes. The conducting aerogels under study complement the well-known set of materials that exhibit hopping electron transport at low temperatures, which is characteristic of media with strong carrier localization, and also a negative magnetoresistance, which usually manifests itself under weak localization conditions.

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