¹National Technical University of Ukraine “Igor Sikorsky Kyiv Polytechnic Institute”
37, prosp. Peremohy, 03056 Kyiv, Ukraine
²Institute of Physics of the CAS, 2 Na Slovance, 182 21 Prague, Czech Republic
³O. Usikov Institute for Radiophysics and Electronics, NAS of Ukraine
12, Proskura str., 61085 Kharkiv, Ukraine
⁴V. Lashkaryov Institute of Semiconductor Physics, NAS of Ukraine
41, prosp. Nauky, 03680 Kyiv, Ukraine
^*Corresponding author e-mail: dariyasavchenko@gmail.com

Abstract. The cadmium manganese telluride (Cd_1–xMn_xTe) crystals (x < 0.001 and x = 0.02, 0.04, 0.1) grown using the Bridgman method were studied by applying continuous wave and pulsed electron paramagnetic resonance (EPR) spectroscopy in the wide temperature range. The Cd1–xMnxTe crystals with x < 0.001 revealed the EPR spectrum from isolated Mn2+ with g⊥ = g∥ = 2.0074(3), |A⊥| = |A∥| = 56.97 ⋅ 10–4 cm–1, |a| = 30.02⋅10–4 cm–1, while Cd1–xMnxTe crystals with x = 0.02…0.04 are characterized by two single broad isotropic EPR lines of Lorentzian shape (g ~ 2.009 and g ~ 1.99) due to Mn clusters of different sizes. The EPR spectrum of Cd_1–xMn_xTe crystals with x = 0.01 consists of the single broad line at g ~ 2.01 due to higher level of homogeneity inherent to these crystals. The temperature dependence of spin relaxation times for the isolated Mn2+ center in the Cd_1–xMn_xTe crystals with x < 0.001 has been described using the conceptions of Orbach process for T_{M^–1 and two-phonon Raman process for T1^–1.}

Keywords: EPR, spin relaxation time, manganese, cadmium manganese telluride.

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