Vibrational-mechanical properties of the highly-mismatched Cd(1−x)Be(x)Te semiconductor alloy: experiment and ab initio calculations

The emerging CdTe–BeTe semiconductor alloy that exhibits a dramatic mismatch in bond covalency and bond stiffness clarifying its vibrational-mechanical properties is used as a benchmark to test the limits of the percolation model (PM) worked out to explain the complex Raman spectra of the related but less contrasted Zn(1−x)Be(x)-chalcogenides. The test is done by way of experiment ([Formula: see text] ), combining Raman scattering with X-ray diffraction at high pressure, and ab initio calculations ([Formula: see text] ~ 0–0.5; [Formula: see text] ~1). The (macroscopic) bulk modulus [Formula: see text] drops below the CdTe value on minor Be incorporation, at variance with a linear [Formula: see text] versus [Formula: see text] increase predicted ab initio, thus hinting at large anharmonic effects in the real crystal. Yet, no anomaly occurs at the (microscopic) bond scale as the regular bimodal PM-type Raman signal predicted ab initio for Be–Te in minority ([Formula: see text] ~0, 0.5) is barely detected experimentally. At large Be content ([Formula: see text] ~1), the same bimodal signal relaxes all the way down to inversion, an unprecedented case. However, specific pressure dependencies of the regular ([Formula: see text] ~0, 0.5) and inverted ([Formula: see text] ~1) Be–Te Raman doublets are in line with the predictions of the PM. Hence, the PM applies as such to Cd(1−x)Be(x)Te without further refinement, albeit in a “relaxed” form. This enhances the model’s validity as a generic descriptor of phonons in alloys.