Continuous wave and pulsed EPR study of Cd1-xMnxTe crystals with different Mn content

D. Savchenko, M.K. Riasna, M. Chursanova, T. V. Matveeva, N. Popenko, I. Ivanchenko, E. Kalabukhova
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Abstract

The cadmium manganese telluride (Cd1–xMnxTe) 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 Cd1–xMnxTe 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 Cd1–xMnxTe crystals with x < 0.001 has been described using the conceptions of Orbach process for TM–1 and two-phonon Raman process for T1–1.
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不同Mn含量Cd1-xMnxTe晶体的连续波和脉冲EPR研究
采用连续波和脉冲电子顺磁共振(EPR)技术,在宽温度范围内研究了Bridgman法生长的碲化镉锰(Cd1-xMnxTe)晶体(x < 0.001和x = 0.02, 0.04, 0.1)。x < 0.001的Cd1-xMnxTe晶体显示了孤立Mn2+的EPR谱,其g⊥= g∥= 2.0074(3),|A⊥| = |A∥= 56.97⋅10-4 cm-1, |A | = 30.02⋅10-4 cm-1,而x = 0.02…0.04的Cd1-xMnxTe晶体由于Mn簇的大小不同,其特征为两条洛伦兹形状的单宽各向同性EPR线(g ~ 2.009和g ~ 1.99)。当x = 0.01时,Cd1-xMnxTe晶体的EPR谱在g ~ 2.01处由一条宽谱线组成,这是由于这些晶体具有较高的均匀性。用奥巴赫过程(TM-1)和双声子拉曼过程(T1-1)描述了x < 0.001的Cd1-xMnxTe晶体中孤立Mn2+中心自旋弛豫时间的温度依赖性。
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