(…)..的超磁相变。陶瓷

F. Bukhanko
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引用次数: 0

摘要

(Sm0.5Gd0.5)0.55Sr0.45MnO3陶瓷的交流磁化率对温度的依赖提供了具有特定量子无序相的混合绝缘状态形成的证据,其中具有远程反铁磁有序的畴在温度低于𝑇N = 48,5 K时占主导地位。在临界场𝐻c1 ~ 25 kOe下,铁磁有序态的不可逆变磁相变在4.2 K ~ 60 K温度范围内保持不变。从磁化等温线的分析可以得出结论,在温度低于临界值𝑇CO ~ 60 K时,可以自发相变到有电荷和轨道有序的状态。假设在𝑇CO以上温度~ 90k的异常大范围内存在短程电荷相关,这大大超过了局部轨道相关的存在面积~ 50k。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Metamagnetic Phase Transitions in (..).. Ceramics
The temperature dependences of ac magnetic susceptibility of the (Sm0.5Gd0.5)0.55Sr0.45MnO3 ceramics provide evidence of the formation of a mixed insulating state with a specific quantum-disordered phase, in which the domains with a long-range antiferromagnetic order dominate at temperatures below 𝑇N≅48,5 K. Irreversible metamagnetic phase transition in the ferromagnetically ordered state is carried out at the critical field 𝐻c1∼25 kOe which remains constant in the temperature range from 4.2 K to 60 K. From the analysis of the magnetization isotherms, the conclusion can be made about a spontaneous phase transition into the state with charge and orbital ordering at temperatures below the critical value 𝑇CO∼60 K. It is supposed that short-range charge correlations exist in unusually large interval of temperatures ~90 K at temperatures above 𝑇CO that considerably exceeds the area of existence of local orbital correlations ~50 K.
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