Table 1 Input parameters involved in the Raman cross section (\(RCS\), Eq. 1) and in the dynamical matrix-elements (\({\widetilde{M}}_{T,L}\), Eqs. 2 and 3) of Cd1−xZnxTe.

From: Taxonomy of high pressure vibration spectra of zincblende semiconductor alloys based on the percolation model

\({Cd}_{1-x}{Zn}_{x}Te\)

Parameters

Pressure dependence (\(P\) in \(GPa\))

\(x = 1\)

\({\omega }_{T} \left({cm}^{-1}\right)\)

\(-0.1474\times {P}^{2} + 5.9742\times P + 176.55\)

(fitted from Ref.38)

\({\omega }_{L} \left({cm}^{-1}\right)\)

\(-0.1172\times {P}^{2} + 4.72464\times P + 205.98\)

(fitted from Ref.38)

\({\varepsilon }_{\infty ,ZnTe}\)

\(7.3\)(Ref.57)

\(x=0\)

\({\omega }_{T} \left({cm}^{-1}\right)\)

\(4.9\times P + 144.4\)

(reconstructed from \({S}_{CdTe}\) measured in this work – see text)

\({\omega }_{L} \left({cm}^{-1}\right)\)

\(4.17\times P + 169.77\)

(fitted from Ref.46)

\({\varepsilon }_{\infty ,CdTe}\)

\(7.1\)(Ref.57)

\(x=0.91\)

\({\omega }_{T,Zn-Te}^{Zn} \left({cm}^{-1}\right)\)

\(4.776\times P + 173.772\)

\({\omega }_{T,Zn-Te}^{Cd} \left({cm}^{-1}\right)\)

\(3.322\times P + 180.039\)

\({x}_{Zn-Te}^{Zn}\)

\({x}^{3}+2\times {x}^{2}\times \left(1-x\right)\)

(taken from Ref.31)

\({x}_{Zn-Te}^{Cd}\)

\({(1-x)}^{2}\times x\)

(taken from Ref.31)

\({\omega }^{{\prime} }\left({cm}^{-1}\right)\)

\(25\)

\(x=0.11\)

\({\omega }_{T,Cd-Te} \left({cm}^{-1}\right)\)

\(-0.48\times {P}^{2} + 7.59\times P + 146\)

\({\omega }_{T,Zn-Te} \left({cm}^{-1}\right)\)

\(7.5\times P + 175\)

\({x}_{Cd-Te}\)

\(1-x\)

\({x}_{Zn-Te}\)

\(x\)