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机构地区:[1]宿州学院材料研究室,宿州234000 [2]中国科学技术大学结构分析开放实验室,合肥230026
出 处:《物理学报》2005年第2期920-929,共10页Acta Physica Sinica
基 金:国家自然科学基金 (批准号 :10 3 3 40 90 );国家重点基础研究发展规划项目 (批准号 :0 0 1CB610 60 4)资助的课题~~
摘 要:通过实验研究了La0 7-xDyxSr0 3MnO3(x =0 0 0 ,0 30 ,0 4 0 ,0 5 0 ,0 6 0 ,0 70 )体系的M_T曲线 ,M_H曲线 ,ρ_T曲线和MR_T曲线 .实验结果表明 :随着Dy掺杂的增加 ,体系从长程铁磁有序向自旋团簇玻璃态、反铁磁及亚铁磁状态转变 .x =0 30样品的M_T曲线上在TN 附近出现磁化强度尖峰 ,x =0 4 0时尖峰消失 .对x =0 5 0样品 ,ZFC的M_T曲线随温度增加出现一个谷 ,随后在TN 处出现峰 ;而FC的M_T曲线在低温下呈现负磁矩 .对x =0 6 0和0 70样品 ,不论FC还是ZFC的M_T曲线都类似于x =0 5 0的ZFC的M_T曲线 .高掺杂时的输运性质在其磁背景下发生异常 .这些奇异现象用N el的双格子模型并联合M_H回滞曲线给予很好地解释 .The M-T curves, M-H curves, rho-T curves and MR-T curves of La0.7-x DyxSr(0.3)MnO(3) (x = 0.00,0.30,0.40,0.50,0.60 and 0.70) are studied. Experimental results indicate that with increasing doping concentration of Dy, the system changes from long-range ferromagnetic order to cluster-spin glass state, then to antiferromagnetic state and to subferromagnetic state. For x = 0.3, there appears a peak on the M-T curve near T-N however, it disappears at x = 0.4. For x = 0.5, and zero field cooling (ZFC) the curve shows a valley, and then a peak at T-N; after the 0.01 T field cooling process, the initial value of M is negative at low temperatures. For x = 0.60 and 0.70, their ZFC and FC M-T curves are both similar to the ZFC one of x = 0.50, and the transport properties at heavy doping become abnormal under a magnetic background. The peculiar phenomena shown above can be interpreted in terms of the Neel's double-lattice model combined with the results of M-H hysteresis at the characteristic temperatures.
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