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Chin. Phys. B, 2011, Vol. 20(11): 117502    DOI: 10.1088/1674-1056/20/11/117502
CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES Prev   Next  

Effects of Fe doping on ac susceptibility of Pr0.75Na0.25MnO3

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)
a College of Science, Northeast Forestry University, Harbin 150040, China; b Post-doctoral Mobile Research Station of Forestry Engineering, Northeast Forestry University, Harbin 150040, China; c Material Science and Engineering College, Northeast Forestry University, Harbin 150040, China
Abstract  Ac susceptibility at low temperatures of Pr$_{0.75}$Na$_{0.25}$Mn$_{1-x}$Fe$_{x}$O$_{3}$ ($0 \le  x \le 0.30$) is investigated. The peak value of the real component of ac susceptibility $\chi '$ at  the freezing  temperature $T_{\rm f }$ is suppressed with the increasing frequency. The peak value of $\chi '$ shows a linear relation between $T_{\rm f}$ and the logarithm of the frequency $\omega$. The normalized slope $P = \Delta T_{\rm  f }/T_{\rm f}\Delta {\rm lg}\omega $, which is much lower than canonical insulating spin glass systems in which $0.06 \le  P \le 0.08$. The peak value of the imaginary component of the ac susceptibility $\chi''$ at $T_{\rm f}$  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 $\chi''$ at $ T_{\rm f}$ for the $x = 0.10$ sample decreases with increasing frequency, suggesting a phase separation ground state. The peak value of $\chi''$ at $ T_{\rm f}$ for the $x = 0.05$ sample decreases with  increasing frequency for $\omega \le 52$ Hz and increases subsequently till 701~Hz, and then decreases with further increasing frequency for $\omega \ge  1501$ 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.
Keywords:  magnetization      ac susceptibility      phase separation      cluster-glass  
Received:  29 August 2011      Revised:  02 September 2011      Accepted manuscript online: 
PACS:  75.50.Lk (Spin glasses and other random magnets)  
  75.60.Ej (Magnetization curves, hysteresis, Barkhausen and related effects)  
  75.30.Kz (Magnetic phase boundaries (including classical and quantum magnetic transitions, metamagnetism, etc.))  
Fund: Project supported by the Fundamental Research Funds for the Central Universities of China (Grant No. DL09BB31), the Open Project of Key Laboratory for Magnetism and Magnetic Materials of the Ministry of Education, Lanzhou University, China (Grant No. LZUMMM2010004),the Fundamental Research Funds for the Central Universities of China (Grant No. DL09BB36), the National Natural Science Foundation of China (Grant No. 31170518), and the Research Fund of Heilongjiang Provincial Education Department (Grant No. 12513040).

Cite this article: 

Li Yu(李玉), Cheng Qian(程倩), Qi Da-Wei(戚大伟), Wang Ji-Liang(王继亮), Zhang Jing(张晶), Wang Shuang(王爽), and Guan Jing(关晶) Effects of Fe doping on ac susceptibility of Pr0.75Na0.25MnO3 2011 Chin. Phys. B 20 117502

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