Lea. Berlouis et al., Surface second harmonic generation in the characterization of anodic sulphide and oxide films on Hg1-xCdxTe (MCT), J ELEC MAT, 28(6), 1999, pp. 830-837
Rotation anisotropy by second harmonic generation (SHG) is carried out on e
pitaxial Hg1-xCdxTe (MCT) and oxide- and sulphide-covered MCT surfaces and
shows the fourfold symmetry pattern expected from the {100} surface (C-4 nu
symmetry). The uneven nature of the four peaks confirm the vicinal surface
obtained from the growth of the MCT on GaAs {100} substrate orientated 4 d
egrees toward the [110] direction. The increase in the SH intensity observe
d for the oxide-covered MCT surface is associated with charge accumulation
at the MCT/oxide interface since the oxide is centrosymmetric and cannot ge
nerate SH. The CdS layer on the other hand is strongly nonlinear active and
generation here comes from a composite of one noncentrosymmetric layer on
top of another. This leads to interactions in the observed SH arising from
the coupling depths (-40 nm) at the two interfaces and from the coherence l
ength (-1200 nm) in the CdS layer. The in-situ SHG measurements during the
growth of the anodic oxide and sulphide layers would suggest that a species
, most likely HgTe is embedded in the anodic layer during the initial stage
s and absorbs the SH radiation at 532 nm. The rotational anisotropy of the
sulphide-covered MCT surface confirms that the CdS layer formed maintains t
he cubic closed pack symmetry of the underlying MCT.