Abstract
In 1930 Shubnikov and de Haas (1) investigated the magnetoresistance of bismuth single crystals at liquid hydrogen temperatures. They observed an oscillatory behavior of the resistance as a function of the magnetic field which was not understood at that time. The foundation for the explanation was laid by Landau (2). Peierls (3) suggested in 1931 that quantum effects might cause the phenomenon. However, not too much attention was paid to the effect, possibly because knowledge of the peculiar behavior was restricted to bismuth for quite some time. Not until 1956 was an oscillatory magnetoresistance, which is now frequently called the Shubnikov-de Haas effect, observed in other substances, in the semiconductor InSb (4) and in Zn (5). Soon experiments on InAs (6,7) followed, and to the present the Shubnikov-de Haas effect has been found in more than a dozen semiconductors. At the end of the 1950’s the first quantitative theories were offered (8–10) which showed much similarity with the theory of the de Haas-Van Alphen effect. Excellent review articles by Kahn and Frederikse (11) and by Adams and Keyes (12) have been published which cover the literature up to about 1961. Consequently, in this chapter emphasis will be on the newer results. In the first section, on oscillatory quantum effects, the theoretical situation will briefly be reviewed, followed by a presentation of recent experimental data.
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Landwehr, G. (1969). The Shubnikov-de Haas Effect and Quantum-Limit Phenomena in Semiconductors. In: Haidemenakis, E.D. (eds) Physics of Solids in Intense Magnetic Fields. Springer, Boston, MA. https://doi.org/10.1007/978-1-4899-5508-1_22
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