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• W2338606700 endingPage "218" @default.
• W2338606700 startingPage "189" @default.
• W2338606700 abstract "The broad classification of materials, by their ability to transport electric current, into metals, semiconductors and insulators, can be generally applied to the same materials when deposited in the form of thin films. It is not then the similarities of films to bulk that give rise to the study of transport properties but the differences between the two, and in particular, the differences that are inherent in the preparation of thin non-metal-lic films. As an example, if we wish to investigate high electric field phenomena, a bulk specimen 10-2m thick would require a power supply capable of giving a potential of 106 volts to give a field of 108 V.m-1, whereas a film 1,000 Å thick only requires 10 V for the same field. A second example is that highly disordered structures can be prepared in the form of thin films by deposition onto cold substrates. Below the deposition temperature these structures are at least metastable and their electrical properties can be investigated. Indeed, without extreme care it is difficult to prepare films which have good crystalline properties and the investigation of transport of charge in non-metallic films is essentially an investigation of the interaction of quasi-mobile charge with the non-crystalline media. Here the first example, of high field, is of interest, for if a non-linear regime of current and voltage can be induced the interaction between electric field and structure can be used to elucidate information about the electronic structure of the material. It is the extraction of this information that is of interest to us here." @default.
• W2338606700 created "2016-06-24" @default.
• W2338606700 creator A5070419474 @default.
• W2338606700 date "1976-01-01" @default.
• W2338606700 modified "2023-09-25" @default.
• W2338606700 title "Electronic Transport Properties" @default.
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• W2338606700 doi "https://doi.org/10.1007/978-1-4684-0847-8_8" @default.
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