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Magnetotransport studies of SiGe-based <i>p</i>-type heterostructures: Problems with the determination of effective mass

I. B. BerkutovB. Verkin Institute for Low Temperature Physics and Engineering , National Academy of Sciences of Ukraine, 47 Lenin Ave., Kharkov 61103, UkraineВ. В. АндриевскииB. Verkin Institute for Low Temperature Physics and Engineering , National Academy of Sciences of Ukraine, 47 Lenin Ave., Kharkov 61103, UkraineYu. F. KomnikB. Verkin Institute for Low Temperature Physics and Engineering , National Academy of Sciences of Ukraine, 47 Lenin Ave., Kharkov 61103, UkraineYu. A. KolesnichenkoB. Verkin Institute for Low Temperature Physics and Engineering , National Academy of Sciences of Ukraine, 47 Lenin Ave., Kharkov 61103, UkraineR. J. H. MorrisDepartment of Physics, University of Warwick , Coventry CV4 7AL, United KingdomD. R. LeadleyDepartment of Physics, University of Warwick , Coventry CV4 7AL, United KingdomO. A. MironovInternational Laboratory of High Magnetic Fields and Low Temperatures , 95 Gajowicka, Wroclaw 53-24, Poland
2012en
ABI

Annotatsiya

The use of Shubnikov-de Haas oscillations for determining effective mass is illustrated by a study of the magnetotransport properties of the two-dimensional hole gas in Si1−xGex (x = 0.13, 0.36, 0.95, 0.98) quantum wells. For some samples the data cannot be fitted to standard theoretical curves in which the scattering of charge carriers is described by the conventional Dingle factor. The reasons for the discrepancies between the experiment the theory are: (i) the effect of spin splitting on the amplitude of the peak in the SdH oscillations; (ii) extra broadening of the Landau levels attributable to an inhomogeneous distribution of the carrier concentration; (iii) the coexistence of short and long-range scattering potentials; and, (iv) population of the second energy level in the quantum well. Ways of calculating the effective hole masses m* for all these cases are presented and values of m* are found for the heterostructures studied here.

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