Abstract

By considering a model in which charge is transported via phonon-induced tunneling of electrons between localized states which are randomly distributed in energy and position, Mott has obtained an electrical conductivity of the form $\ensuremath{\sigma}\ensuremath{\propto}\mathrm{exp}[\ensuremath{-}{(\frac{\ensuremath{\lambda}{\ensuremath{\alpha}}^{3}}{{\ensuremath{\rho}}_{0}\mathrm{kT}})}^{\frac{1}{4}}]$. Here $T$ is the temperature of the system, ${\ensuremath{\rho}}_{0}$ is the density of states at the Fermi level, $\ensuremath{\lambda}$ is a dimensionless constant, and ${\ensuremath{\alpha}}^{\ensuremath{-}1}$ is the distance for exponential decay of the wave functions. We rederive these results, relating $\ensuremath{\lambda}$ to the critical density of a certain dimensionless percolation problem, and we estimate $\ensuremath{\lambda}$ to be approximately 16. The applicability of the model to experimental observations on amorphous Ge, Si, and C is discussed.

Keywords

PhysicsDimensionless quantityCondensed matter physicsLambdaQuantum tunnellingFermi energyDensity of statesEnergy (signal processing)ElectronPercolation (cognitive psychology)Quantum mechanics

Affiliated Institutions

Related Publications

Publication Info

Year
1971
Type
article
Volume
4
Issue
8
Pages
2612-2620
Citations
1875
Access
Closed

Social Impact

Social media, news, blog, policy document mentions

Citation Metrics

1875
OpenAlex
29
Influential
1760
CrossRef

Cite This

Vinay Ambegaokar, B. I. Halperin, J. S. Langer (1971). Hopping Conductivity in Disordered Systems. Physical review. B, Solid state , 4 (8) , 2612-2620. https://doi.org/10.1103/physrevb.4.2612

Identifiers

DOI
10.1103/physrevb.4.2612

Data Quality

Data completeness: 77%