2006
DOI: 10.1016/j.jnoncrysol.2006.01.057
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The localization of electrons in amorphous semiconductors: A twenty-first century perspective

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Cited by 16 publications
(12 citation statements)
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“…The electron-phonon interaction is so strong that a local change of charge of an atom tends to promote, within a time of the inverse of a phonon frequency, a change in local bonding, if allowed by the open structure of the material. Such lattice relaxation overcomes the Coulomb repulsion and allows the placement of two electrons on one defect [8]. The result is a negative effective correlation energy −U with unusual consequences for the defect chemistry of chalcogenides glasses: there are no singly occupied natural defects detectable by ESR [9].…”
Section: Original Papermentioning
confidence: 99%
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“…The electron-phonon interaction is so strong that a local change of charge of an atom tends to promote, within a time of the inverse of a phonon frequency, a change in local bonding, if allowed by the open structure of the material. Such lattice relaxation overcomes the Coulomb repulsion and allows the placement of two electrons on one defect [8]. The result is a negative effective correlation energy −U with unusual consequences for the defect chemistry of chalcogenides glasses: there are no singly occupied natural defects detectable by ESR [9].…”
Section: Original Papermentioning
confidence: 99%
“…These are not as effective for pinning E f as dispersed members of VAPs because interconverting a positive defect into a negative one in intimate vicinity of a negative defect is energetically not so favorable. Taylor pointed out that the effective correlation energy U does not remain negative for all alloy concentrations containing chalcogenides [8]. U tends to become positive below certain chalcogen concentrations in the alloy.…”
Section: Original Papermentioning
confidence: 99%
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“…This figure also demonstrates that these residual carriers can be freed by excitation with IR light which, switched on after a dark period t D , causes a rapid decrease of the residual LESR signal and the generation of transient photoconductivity and photoluminescence. Taylor demonstrated in his Mott Lecture at ICANS 21 that such long-time decays of band-tail carriers are a quite universal feature observable in many disordered materials [28].…”
Section: Recombination Kinetics: Geminate and Non-geminate Recombinationmentioning
confidence: 99%
“…Surprisingly, the transport (trapping and recombination) in a-Si:H and μc-Si:H is better understood at low temperatures [8,9], while room-temperature operation is of interest for real-life devices.…”
Section: Introductionmentioning
confidence: 99%