Universal conductance fluctuations

Universal conductance fluctuations (UCF) in quantum physics is a phenomenon encountered in electrical transport experiments in mesoscopic species. The measured electrical conductance will vary from sample to sample, mainly due to inhomogeneous scattering sites. Fluctuations originate from coherence effects for electronic wavefunctions and thus the phase-coherence length $\textstyle l_\phi$ needs be larger than the momentum relaxation length $\textstyle l_m$ . UCF is more profound when electrical transport is in weak localization regime. $\textstyle l_\phi<l_c$ where $l_c=M\times l_m$ , $\textstyle M$ is the number of conduction channels and $\textstyle l_m$ is the momentum relaxation length or mean free path. For weakly localized samples fluctuation in conductance is equal to fundamental conductance $\textstyle G_o=2e^2/h$ regardless of the number of channels.

References

Akkermans and Montambaux, Mesoscopic Physics of Electrons and Photons, Cambridge University Press (2007)
S. Datta, Electronic Transport in Mesoscopic Systems, Cambridge University Press (1995)
R. Saito, G. Dresselhaus and M. S. Dresselhaus, Physical Properties of Carbon Nanotubes, Imperial College Press (1998)
Lee, P.; Stone, A. (1985). "Universal Conductance Fluctuations in Metals". Physical Review Letters 55 (15): 1622–1625. Bibcode:1985PhRvL..55.1622L. doi:10.1103/PhysRevLett.55.1622. PMID 10031872.
Altshuler, B. L. (1985), Pis'ma Zh. Eksp. Teor. Fiz. 41: 530 [JETP Lett. 41: 648] ^[1]

References

↑ Fluctuations in the extrinsic conductivity of disordered conductors, Al'tshuler B. L., VOLUME 41, ISSUE 12, PAGE 648, JETP Letters

Universal conductance fluctuations

See also

References

References