TUNNELING AND HOPPING BETWEEN DOMAINS IN THE METAL-INSULATOR TRANSITION IN TWO-DIMENSIONS (Articolo in rivista)

Type
Label
  • TUNNELING AND HOPPING BETWEEN DOMAINS IN THE METAL-INSULATOR TRANSITION IN TWO-DIMENSIONS (Articolo in rivista) (literal)
Anno
  • 2008-01-01T00:00:00+01:00 (literal)
Alternative label
  • Neilson, D; Hamilton, A (2008)
    TUNNELING AND HOPPING BETWEEN DOMAINS IN THE METAL-INSULATOR TRANSITION IN TWO-DIMENSIONS
    in International journal of modern physics b
    (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#autori
  • Neilson, D; Hamilton, A (literal)
Pagina inizio
  • 4565 (literal)
Pagina fine
  • 4571 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroVolume
  • 22 (literal)
Rivista
Note
  • ISI Web of Science (WOS) (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#affiliazioni
  • \"[Neilson, David] Univ Camerino, Dipartimento Fis, I-62032 Camerino, Italy; [Neilson, David] NEST CNR INFM, I-56126 Pisa, Italy; [Neilson, David; Hamilton, Alex] Univ New S Wales, Sch Phys, Sydney, NSW 2052, Australia (literal)
Titolo
  • TUNNELING AND HOPPING BETWEEN DOMAINS IN THE METAL-INSULATOR TRANSITION IN TWO-DIMENSIONS (literal)
Abstract
  • Motivated by recent surprising experimental results for temperature dependent resistivities in 2D mesoscopic electron systems, we investigate transport in these systems by percolation connected through a network of metallic domains. The size of the domains is determined by the level of disorder in the system and by the strength of the electron correlations. In the insulating phase the metallic domains are connected for transport by two competing mechanisms, thermally activated hopping and quantum tunneling. We calculate the transmission across the potential barriers that separate the metallic domains. Using recent data from transport measurements in mesoscopic 2D systems, we obtain the observed saturation of the temperature dependent resistivity at T similar to 1 K and consistent values for the size of the domains and for magnitude of the average variation in the random potential. (literal)
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