Damage-induced changes in the electronic properties of InSb(100): implications for surface preparation
W T Yuen; M O Schweitzer; T S Jones; C F McConville; E A Johnson; A Mackinnon; N V Richardson; R A Stradling; W T Yuen; Dept. of Phys., Imperial Coll., London, UK; M O Schweitzer; Dept. of Phys., Imperial Coll., London, UK; T S Jones; Dept. of Phys., Imperial Coll., London, UK; C F McConville; Dept. of Phys., Imperial Coll., London, UK; E A Johnson; Dept. of Phys., Imperial Coll., London, UK; A Mackinnon; Dept. of Phys., Imperial Coll., London, UK; N V Richardson; Dept. of Phys., Imperial Coll., London, UK; R A Stradling; Dept. of Phys., Imperial Coll., London, UK
Журнал:
Semiconductor Science and Technology
Дата:
1993-01-01
Аннотация:
A combination of surface-sensitive techniques and electron transport measurements have been used to characterize the effect of argon ion bombardment and annealing on a series of InSb(100) samples. Ex situ electrical conductivity and magnetoresistance measurements at 4.2 K, and in situ high-resolution electron energy loss spectroscopy (HREELS) carried out at 300 K, indicate that all the samples studied exhibit enhanced n-type behaviour after the surface cleaning procedure. This effect is most pronounced after annealing to between 450 and 500 K and arises from the formation of a high-density electron gas with a sheet carrier concentration of approximately (6.5-9.0)*10<sup>12 </sup>cm<sup>-2</sup>. The carrier concentration is significantly reduced on annealing to higher temperatures up to a maximum of 700 K. Electron-energy-dependent HREELS measurements of the plasmon energy and intensity, in conjunction with model calculations based on dielectric theory, indicate that the n-type layer is approximately 500 AA thick and located approximately 175 AA below a surface depletion layer. The occupancy of the electronic subbands has been obtained by Shubnikov-de Haas measurements and self-consistent calculations. These show that the positive charge which confines the electrons is spread over approximately 300 AA with a best fit being provided by a Gaussian-like potential profile. The calculations demonstrate that the corresponding wavefunction spread for the i=0 subband, which contains approximately 40% of the total carriers induced, has a spatial dimension of approximately 500 AA in good agreement with the HREELS results.
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