Electrical and magnetic properties of Y-doped La0.5Sr0.5MnO3 manganite system: Observation of step-like magnetization

被引:8
作者
Taran, Subhrangsu [1 ]
Sun, C. P. [2 ]
Huang, C. L. [2 ]
Yang, H. D. [2 ]
Nigam, A. K. [3 ]
Chaudhuri, B. K. [4 ]
Chatterjee, S. [5 ]
机构
[1] Kalyani Mahavidyalaya, Dept Phys, Nadia 741235, W Bengal, India
[2] Natl Sun Yat Sen Univ, Dept Phys, Ctr Nanosci & Nanotechnol, Kaohsiung 804, Taiwan
[3] Tata Inst Fundamental Res, Dept CMP & MS, Bombay 400005, Maharashtra, India
[4] Indian Assoc Cultivat Sci, Dept Solid State Phys, Kolkata 700032, India
[5] Banaras Hindu Univ, Indian Inst Technol, Dept Appl Phys, Varanasi 221005, Uttar Pradesh, India
关键词
Manganites; Structural properties; Magnetic relaxation; SPIN-GLASS INSULATOR; PHASE-SEPARATION; SIZE MISMATCH; TRANSITION; FIELD; METAL; PR; MAGNETORESISTANCE; DISORDER; STATE;
D O I
10.1016/j.jallcom.2015.05.050
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The magnetic and transport properties of bulk doped manganite, La0.5-yYySr0.5MnO3 have been studied as a function of (Y) yttrium doping, y, for 0 <= y <= 0.25. In the absence of the yttrium this is a well studied half-doped manganite which is a metallic ferromagnet. With successive doping of Y the system undergoes a transformation from rhombohedral (space group R (3) over bar - C) to orthorhombically (space group Pnma) distorted perovskite structure, due to the large distortions caused by the yttrium; this is seen directly from the softening of the Mn-O stretching mode (around 600 cm(-1)) as a function of Y3+ doping which has relatively lower ionic radius compared to La3+ and Sr2+. These distortions make this series of compounds particularly interesting. The magnetization obtained in zero field cooled (ZFC) and field cooled (FC) studies show dramatic changes as the value of y is raised above 0.05. This is accompanied by a transition from the metallic and into a semiconducting state as is seen from the studies of the electrical resistivity. The magnetic behavior is further investigated by a study of the hysteresis loops, frequency dependent susceptibility and studies of the magnetic relaxation. The results are understood in terms of the average size of the cation on the A site, < r(A)>, and the variance, sigma(2) (=Sigma y(i)(2)r(i)(2) - < r(A)>(2)) The value of the variance, sigma(2), increases rapidly with doping, y, induces weakening of the long range ferromagnetic ordering, exhibiting a stepwise variation of magnetization (metamagnetic like). Based on the present results a magnetic phase diagram has been drawn demonstrating different magnetic phase sequences with the variation of sigma(2). (C) 2015 Elsevier B.V. All rights reserved.
引用
收藏
页码:363 / 370
页数:8
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