中国物理B ›› 2011, Vol. 20 ›› Issue (11): 117502-117502.doi: 10.1088/1674-1056/20/11/117502
王继亮1, 张晶1, 王爽1, 关晶1, 李玉2, 戚大伟2, 程倩3
Li Yu(李玉)a)b), Cheng Qian(程倩)c), Qi Da-Wei(戚大伟)a)b)†, Wang Ji-Liang(王继亮)a), Zhang Jing(张晶)a), Wang Shuang(王爽)a), and Guan Jing(关晶)a)
摘要: Ac susceptibility at low temperatures of Pr0.75Na0.25Mn1-xFexO3 (0 ≤ x ≤ 0.30) is investigated. The peak value of the real component of ac susceptibility χ' at the freezing temperature Tf is suppressed with the increasing frequency. The peak value of χ' shows a linear relation between Tf and the logarithm of the frequency ω. The normalized slope P = ΔTf/TfΔlgω, which is much lower than canonical insulating spin glass systems in which 0.06 ≤ P ≤ 0.08. The peak value of the imaginary component of the ac susceptibility χ'' at Tf for the x = 0, 0.02, 0.30 samples increases with increasing frequency, suggesting a cluster glass ground state with a coexistence of charge-ordered phase and correlated ferromagnetic clusters in spin glass matrix. The peak value of χ'' at Tf for the x = 0.10 sample decreases with increasing frequency, suggesting a phase separation ground state. The peak value of χ'' at Tf for the x = 0.05 sample decreases with increasing frequency for ω ≤ 52 Hz and increases subsequently till 701 Hz, and then decreases with further increasing frequency for ω ≥ 1501 Hz. This complex behaviour is ascribed to the competition between the effects of large and little ferromagnetic clusters in the sample. The ground state of x = 0.05 sample is a transition state from cluster glass to phase separation.
中图分类号: (Spin glasses and other random magnets)