We report the results of a spin-flip Raman scattering study of electrons bound to shallow donors in the diluted magnetic semiconductors Cd_1-x{Mn}ₓ$Te and ${Cd}_{1{{-}}x}MnₓSe for x{}0.30 and in Cd_1-x{Mn}ₓ$S for x=0.022 and 0.125. Spin-flip Raman scattering is observed at temperatures ranging from 1.8 K to as high as 160 K and at magnetic fields {≤}60 kG. The measured spin-flip energies are large and, for some samples, correspond to g values in excess of 100 at low temperatures. The enhancement of the Raman shifts results from the exchange coupling of the donor electron with the Mn²⁺ ions. The parameters of the mean-field approximation, used to describe the magnetic field and temperature dependence of g are shown to exhibit a temperature dependence for temperatures above 20 K. Finite Raman shifts are observed in the absence of a magnetic field and are attributed to the bound magnetic polaron and thermal fluctuations of the local magnetization. The temperature and magnetic field dependences of the spin-flip energies, Raman intensities, and polarizations were compared with the results of the statistical-mechanical model of Dietl and Spal/ek [Phys. Rev. B 28, 1548 (1983)]. The theory is in good agreement with the experimental results for x{}0.15.
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Peterson et al. (1985) studied this question.
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