Conduction mechanism studies on electron transfer of disordered system

Hui Xu , Yi-pu Song , Xin-mei Li

Journal of Central South University ›› 2002, Vol. 9 ›› Issue (2) : 134 -137.

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Journal of Central South University ›› 2002, Vol. 9 ›› Issue (2) : 134 -137. DOI: 10.1007/s11771-002-0058-3
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Conduction mechanism studies on electron transfer of disordered system

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Abstract

Using the negative eigenvalue theory and the infinite order perturbation theory, a new method was developed to solve the eigenvectors of disordered systems. The result shows that eigenvectors change from the extended state to the localized state with the increase of the site points and the disordered degree of the system. When electric field is exerted, the electrons transfer from one localized state to another one. The conductivity is induced by the electron transfer. The authors derive the formula of electron conductivity and find the electron hops between localized states whose energies are close to each other, whereas localized positions differ from each other greatly. At low temperature the disordered system has the character of the negative differential dependence of resistivity and temperature.

Keywords

disordered system / localized state / electron transfer / D. C. conductivity

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Hui Xu, Yi-pu Song, Xin-mei Li. Conduction mechanism studies on electron transfer of disordered system. Journal of Central South University, 2002, 9(2): 134-137 DOI:10.1007/s11771-002-0058-3

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References

[1]

MottN F, DavisE AElectronic processes in non-crystalline Materials[M], 1979, London, Clarendon Press

[2]

MillerA, AbrahamsE. Impurity conduction at low concentrations[J]. Phys Rev, 1960, 120(6): 745-756

[3]

AldeaA, et al.. Hopping conduction on aperiodic chains[J]. Phys Rev Lett, 1988, 60: 1672-1674

[4]

NewmanM E J, et al.. Hopping conductivity of the fibonaccichain quasicrystal[J]. Phys Rev B, 1991, 43(1): 1183-1191

[5]

MandelbrotB BThe fractal geometry of nature[M], 1982, San Francisco, Freeman

[6]

SamukhinA N, et al.. Hopping conductivity of a nearly 1D fractal: A model for conductingpolymers[J]. Phys Rev B, 1998, 58(17): 11354-11362

[7]

AndersonP W. Absence of diffusion in certain random lattices[J]. Phys Rev, 1958, 109(5): 1492-1505

[8]

DeanP, MartinJ L. Frequency spectra of disordered lattices in two-dimensions[J]. Proc Roy Soc, 1960, A259: 409-417

[9]

WuS Y, ZhengZ B. Applications of infinite order perturbation theory[J]. Phys Rev B, 1981, 24: 4787-4796

[10]

XuHui. The solution of the eigenvectors in one dimensional disordered system[J]. Journal of Computational Physics, 1991, 8(3): 295-304(in Chinese)

[11]

RiccoB, AzbelM Ya. Physics of resonant tunneling: the one dimensional double-barriercase[J]. Phys Rev B, 1984, 29(4): 1970-1981

[12]

AzbelM Ya. Eigenstates and properties of random system in one dimension at zero temperature[J]. Phys Rev B, 1983, 28(8): 4106-4125

[13]

SavvidesN, McAlisterS P, HurdC M, et al.. Localization in the metallic regime of granular Cu-SiO2 films[J]. Solid State Commun, 1982, 42(2): 143-145

[14]

XiaY, BhattacharyaS, PonnambalamV. Thermoelectric properties of semimetallic CoSb half-Heusler phases [J]. Journal of applied physics, 2000, 88(4): 1952-1955

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