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首页> 外文期刊>Journal of Applied Physics >Structural phase transitions of robust insulating Bi_(1-x)La_xFe_(1-y)Ti_yO_3 multiferroics
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Structural phase transitions of robust insulating Bi_(1-x)La_xFe_(1-y)Ti_yO_3 multiferroics

机译:坚固的绝缘Bi_(1-x)La_xFe_(1-y)Ti_yO_3多铁化合物的结构相变

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摘要

In contrast to leaky BiFeO_3, of which two structural phase transitions of cycloidal modulated antiferromagnetic-paramagnetic and ferroelectric-paraelectric are observed below 850 ℃, chemical co-substitution to form Bi_(1-x)La_xFe_(1-y)Ti_yO_3 ternary solid solution makes these multiferroic ceramics become robust insulating low dielectric loss and exhibit rich structural phase transitions. Differential thermal analysis and temperature-dependent X-ray diffraction measurements probe four first-order structural phase transitions, e.g., T_H = 305℃, T_N = 365℃, T_C = 810℃, and T_S = 830℃ observed in the Bi_(0.98)La_(0.02)Fe_(0.99)Ti_(0.01)O_3 system, which are reasonably attributed to Brazovskii-type cycloidal modulated antiferromagnetic-helimagnetic (at T_H) and helimagnetic-paramagnetic (at T_N) magnetic phase transitions, ferroelectric-paraelectric (at T_C) and rhombohedral-cubic (at T_S) structural phase transitions, respectively. Magnetic phase transition temperatures change a little but ferroelectric and lattice structural phase transition temperatures decrease gradually with increasing co-substitution up to composition-induced rhombohedral-(pseudo-)cubic structural phase boundary. The first-order nature of magnetic phase transition and emergence of helimagnetic phase were attributed to Ti~(3+) d~1 magnetic disorder distribution in the Fe~(3+) d~5-O-Fe~(3+) d~5 chains, while the first-order nature becomes weak with increasing co-substitution, owing to decreased ferroelectric rhombohedral lattice distortion. An intermediate rhombohedral paraelectric phase is discovered intervening between ferroelectric rhombohedral and paraelectric cubic phase, of which the temperature range defined by difference between T_C and T_S increases with increasing co-substitution. It was found that T_C and T_S are able to be predicted quantitatively by reduced mass of unit cell. These findings enrich our understanding of ferroic phase transitions and advance designing novel high temperature multiferroic compounds.
机译:与泄漏的BiFeO_3不同,在850℃以下会观察到摆线调制的反铁磁-顺磁和铁电-顺电的两个结构相变,化学共取代形成Bi_(1-x)La_xFe_(1-y)Ti_yO_3三元固溶体使这些多铁性陶瓷成为坚固的绝缘材料,介电损耗低,并呈现出丰富的结构相变。差热分析和随温度变化的X射线衍射测量可探测到在Bi_(0.98)中观察到的四个一级结构相变,例如T_H = 305℃,T_N = 365℃,T_C = 810℃和T_S = 830℃。 La_(0.02)Fe_(0.99)Ti_(0.01)O_3系统,合理地归因于Brazovskii型摆线调制反铁磁-顺磁(T_H)和日磁-顺磁(T_N)磁相变,铁电-顺电(T_C) )和菱形-立方(在T_S处)结构相变。磁相变温度略有变化,但铁电和晶格结构相变温度随着共取代的增加而逐渐降低,直至成分诱导的菱面体-(伪)立方结构相界。 Fe〜(3+)d〜5-O-Fe〜(3+)d中的Ti〜(3+)d〜1磁性无序分布归因于磁性相变的一级性质和螺旋相的出现。 〜5条链,但由于铁电菱面体晶格畸变的减少,一阶性质随着共取代的增加而变弱。发现在铁电菱形面相和顺电立方相之间存在中间的菱面体顺电相,其温度范围由T_C和T_S之间的差定义,随共取代的增加而增加。已经发现,通过降低单位晶胞的质量可以定量地预测T_C和T_S。这些发现丰富了我们对铁相变的理解,并进一步设计了新颖的高温多铁化合物。

著录项

  • 来源
    《Journal of Applied Physics》 |2014年第12期|123523.1-123523.8|共8页
  • 作者单位

    Functional Materials Research Laboratory, Tongji University, Shanghai 200092, China;

    Functional Materials Research Laboratory, Tongji University, Shanghai 200092, China;

    Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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