Md. Sciacca et al., HOST-ISOTOPE FINE-STRUCTURE OF LOCAL AND GAP MODES OF SUBSTITUTIONAL IMPURITIES IN ZINCBLENDE AND WURTZITE II-VI SEMICONDUCTORS, Physical review. B, Condensed matter, 53(19), 1996, pp. 12878-12883
The frequency of a local vibrational mode (LVM) of a light impurity su
btituting for either the group II or the group VI host atom in a II-VI
semiconductor (e.g., Mg2+ replacing Zn2+ in ZnTe) exhibits two types
of isotope shifts: in one, the shift is caused by the specific isotope
of the impurity, whereas in the other a shift occurs in association w
ith the isotopes of the nearest neighbor (NN) atoms of the impurity, T
e in the above case. Depending on the number of isotopes of host atoms
, a variety of isotopic configurations in the surrounding ''cage'' of
NN's can occur. The striking similarity of this host-isotopic fine str
ucture for the same type of NN's (e.g., Te in ZnTe and CdTe), irrespec
tive of the impurity (X) and its isotopes, justifies the LVM to be ass
ociated with the high-frequency, infrared active, triply degererate (G
amma(5)) mode of an XY(4) molecule, the four Y's being the NN's. A num
erical calculation of the normal modes of such an XY(4) molecule, usin
g stretching and bending force constants, reproduces the entire host-i
sotope fine structure of an LVM with remarkable fidelity when all the
isotopic NN combinations are appropriately taken into account. When th
e impurity has a mass such that in addition to a local mode a gap mode
results, the numerical calculations correctly predict the absence of
observable isotopic shifts in the gap mode ascribed to the lower-frequ
ency Gamma(5) mode. When the substitutional impurity replaces the ligh
ter host atom (while being heavier), the local mode is absent and only
a gap mode can occur and can be associated with the high-frequency Ga
mma(5). If only a gap mode is to be expected as for Se2- in ZnS, both
computer calculation as well as experimental observation display strik
ing isotopic shifts associated with both the impurity and the host ato
ms. The model also satisfactorily describes the anisotropic effects fo
r an LVM in a wurtzite host (e.g., Mg2+ in CdSe).