1969
DOI: 10.1002/pssb.19690350125
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Cyclotron Resonance in Tellurium

Abstract: Cyclotron resonance of electrons and holes has been observed in tellurium single crystals a t 24 and 70 GHz and at liquid helium temperatures. In pure specimens and a t low temperatures the surfaces of constant energy for the holes are well described by 4 prolate ellipsoids of revolution about the c-axis located near the Brillouin Zone corners. At higher hole energies produced by thermal or optical excitation or by heavily doping the crystals, pairs of t.hese ellipsoidal surfaces degenerate into dumbbell-shape… Show more

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Cited by 17 publications
(5 citation statements)
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“…The agreement between our experimental results and the description of the conduction band by the Bangert model should be a hint that the electrons of interest in our experiment are located near the point H in the Brillouin zone and not in point Z as assumed by Radoff and Dexter [12].…”
Section: Cobiduction Bandsupporting
confidence: 85%
“…The agreement between our experimental results and the description of the conduction band by the Bangert model should be a hint that the electrons of interest in our experiment are located near the point H in the Brillouin zone and not in point Z as assumed by Radoff and Dexter [12].…”
Section: Cobiduction Bandsupporting
confidence: 85%
“…The present results give further evidence of the existence of a second conduction band minimum in Te (Fig. 5), which is also indicated by the cyclotron resonance data of Radoff and Dexter [30]. However, a satisfying agreement between theoretical and experimental transport properties, according t o Link [29], is only obtained when an infinite electron mass in the upper conduction band is assumed.…”
Section: Intrinsic Conductionsupporting
confidence: 76%
“…In the corresponding random ferromagnet 2 only a fraction p of the lattice sites are occupied with Ising spins, the rest remaining vacant, and exchange interactions exist only between spins on neighboring pairs of occupied sites. 3 It is shown that in a class of randomly diluted Ising ferromagnets the magnetization fails to be an analytic function of the field H at #= 0 for a range of temperatures above that at which spontaneous magnetization first appears.…”
mentioning
confidence: 99%