Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
7998484 | Journal of Alloys and Compounds | 2015 | 8 Pages |
Abstract
The magnetic and transport properties of bulk doped manganite, La0.5âyYySr0.5MnO3 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 R3¯-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 cmâ1) 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, ãrAã, and the variance, Ï2 (=âyi2ri2 â ãrAã2). The value of the variance, Ï2, 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 Ï2.
Related Topics
Physical Sciences and Engineering
Materials Science
Metals and Alloys
Authors
Subhrangsu Taran, C.P. Sun, C.L. Huang, H.D. Yang, A.K. Nigam, B.K. Chaudhuri, S. Chatterjee,