文摘
The low field magnetization-step effect was observed in the spin-glass (SG) regime of p-type line-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Hg0.8line-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Mn0.2line-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML" mathvariant="normal">Te single crystal when the temperature was less than about 3 K. The main features of this effect were (i) the magnetic susceptibility suddenly reduced to almost zero as the magnetic field decreased below a critical value; (ii) the critical magnetic field correlated reversely to temperature. In addition, X-ray diffraction, Raman scattering, and temperature-dependent Hall measurements manifested this effect was the intrinsic nature of the line-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Hg1−xline-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Mnxline-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML" mathvariant="normal">Te single crystal. Qualitative theoretical analysis suggests that the possible mechanism of low field magnetization-step effect is the combined effect of SG transition and (long-range) antiferromagnetic interactions among line-library/content/render" xmlns="http://www.w3.org/1998/Math/MathML">Mn2+ ions in randomly frustrated spins system.