首页> 外文期刊>Magnetics, IEEE Transactions on >Electrical and Magnetotransport Properties of ${rm La}_{{0.7}}{rm Ca}_{{0.3}}{rm Mn}_{{1-x}}{rm Co}_{{x}}{rm O}_{3}$
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Electrical and Magnetotransport Properties of ${rm La}_{{0.7}}{rm Ca}_{{0.3}}{rm Mn}_{{1-x}}{rm Co}_{{x}}{rm O}_{3}$

机译:$ {rm La} _ {{0.7}} {rm Ca} _ {{0.3}} {rm Mn} _ {{1-x}} {rm Co} _ {{x}} {rm的电和磁传输性质O} _ {3} $

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This paper presents a detailed study on the Co-doping influence on the electrical and magnetotransport properties of ${rm La}_{0.7}{rm Ca}_{0.3}{rm Mn}_{1-x}{rm Co}_{x}{rm O}_{3}(x={0.09}{-}0.17)$ prepared by solid-state reaction. Magnetic measurements versus temperature revealed a gradual decrease of the magnetization $(M)$ and Curie temperature $(T_{C})$ with increasing Co concentration $(x)$ . The $T_{C}$ values vary from 194 to 159 K as changing $x$ from 0.09 to 0.17, respectively. $H/M$ versus $M^{2}$ performances around $T_{C}$ prove the $x={0.09}$ sample undergoing a first-order magnetic phase transition (FOMT) while the samples with $xgeq 0.11$ undergo a second-order magnetic phase transition (SOMT). The other with $x={0.10}$ is considered as a threshold concentration of the FOMT–SOMT transformation. Considering temperature dependences of resistivity, $rho(T)$ , in the presence and absence of the magnetic field, the samples (excepting for $x={rm 0.17}$ ) exhibit a metal- –insulator transition at $T_{P}=60{-}160~{rm K}$ , which shifts toward lower temperatures with increasing $x$ . In the metallic-ferromagnetic region, the $rho(T)$ data are well fitted to a power function $rho(T)=rho_{0}+rho_{2}T^{2}+rho_{4.5}T^{4.5}$ . This indicates electron–electron and electron–magnon scattering processes are dominant at temperatures $Ttheta_{D}/2$ ( $theta_{D}$ is the Debye temperature) and $T_{P}
机译:本文详细研究了共掺杂对$ {rm La} _ {0.7} {rm Ca} _ {0.3} {rm Mn} _ {1-x} {rm Co}的电和磁传输性质的影响。通过固态反应制备的_ {x} {rm O} _ {3}(x = {0.09} {-} 0.17)$。磁测量值与温度的关系表明,随着Co浓度$(x)$的增加,磁化强度$(M)$和居里温度$(T_ {C})$逐渐降低。当$ x $从0.09变为0.17时,$ T_ {C} $的值从194变为159K。 $ H / M $与$ M ^ {2} $在$ T_ {C} $附近的性能证明$ x = {0.09} $的样本经历了一阶磁相变(FOMT),而具有$ xgeq的样本为0.11 $经历二阶磁性相变(SOMT)。 $ x = {0.10} $的另一个被认为是FOMT-SOMT转换的阈值浓度。考虑到在存在和不存在磁场的情况下电阻率$ rho(T)$的温度依赖性,样品($ x = {rm 0.17} $除外)在$ T_ {P}处表现出金属-绝缘体转变= 60 {-} 160〜{rm K} $,随着$ x $的增加,温度逐渐降低。在金属铁磁区域中,$ rho(T)$数据很好地拟合到幂函数$ rho(T)= rho_ {0} + rho_ {2} T ^ {2} + rho_ {4.5} T ^ { 4.5} $。这表明在温度$ T theta_ {D} / 2 $($ theta_ {D} $是德拜温度)和$ T_ {P}

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