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首页> 外文期刊>IEEE Transactions on Magnetics >Unusual Critical Behavior in La1.2Sr1.8Mn2O7Single Crystal
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Unusual Critical Behavior in La1.2Sr1.8Mn2O7Single Crystal

机译:La 1.2 Sr 1.8 Mn 2 O 7 单晶的异常临界行为

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In this paper, we present a detailed analysis on the critical behavior of La1.2Sr1.8Mn2O7single crystal via isothermal magnetization measured at different temperatures around the paramagnetic-ferromagnetic phase transition at TC= 85 K. Using the Landau-Lifshitz coefficients, the Arrott plots (H/M = a(T) + b(T)M2) of sample have been analyzed. It showed that a(T) changed from positive to negative values at different temperatures in the field ranges of H = 0-10, 10-30, and 30-50 kOe, indicating that the critical behavior could not be described with a single model under different applied fields. Through the modified Arrott plots method, the Kouvel-Fisher method, and the critical isotherm analysis, we determined the values of the critical exponents for La1.2Sr1.8Mn2O7around its magnetic phase transition over different magnetic field ranges. The critical exponent β value is found to be 0.501, 0.417, and 0.371 under field ranges of H = 0-10, 10-30, and 30-50 kOe, respectively. This means that the β value depends strongly on the strength of the applied field, shifting from the value approaching that of the mean field model (β = 0.5) to the 3-D-Heisenbeg model (β = 0.365). Meanwhile, its y value is quite stable (γ = 0.973-1.074), almost independent on the choice of field fitting range. In addition, using the reduced temperature ε = (T - T )/T and the obtained critical exponents, almost M(H, T) data measured near T obey the scaling equation M(H, e) = eβ f±(H/eβ+γ), where f+and f-are regular analytic functions corresponding to data at T > TCand T <; TC, respectively.
机译:在本文中,我们对La n 1.2Sr 1.8 nMn n 2 nO n 7 ns单晶通过等温磁化强度在顺磁性周围的不同温度下测量T n C n = 85K。使用Landau-Lifshitz系数,得出Arrott图(H / M = a(T)+ b(T)M n 2 n)已经分析过了。结果表明,在H = 0-10、10-30和30-50 kOe的磁场范围内,在不同温度下a(T)从正值变为负值,这表明无法用单个模型来描述临界行为。在不同的应用领域下。通过改进的Arrott图方法,Kouvel-Fisher方法和临界等温线分析,我们确定了La n 1.2 nSr n 1.8 nMn n 2 nO n <子xmlns:mml = “ http://www.w3.org/1998/Math/MathML ” xmlns:xlink = “ http://www.w3.org/1999/xlink ”> 7 在不同磁场范围内其磁相变附近。发现在H = 0-10、10-30和30-50 kOe的磁场范围内,临界指数β值分别为0.501、0.417和0.371。这意味着β值在很大程度上取决于所施加场的强度,从接近于平均场模型(β= 0.5)的值转变为3-D-海森贝格模型(β= 0.365)。同时,其y值相当稳定(γ= 0.973-1.074),几乎与场拟合范围的选择无关。此外,使用降低的温度ε=(T-T)/ T和获得的临界指数,在T附近测得的几乎M(H,T)数据服从比例方程M(H,e)=eβf n ± n(H / e n β+γ n),其中f n +和f n - 没有对应于T> T n C nand T <; T n C n。

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