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Anomalous temperature and field behaviors of magnetization in cubic lattice frustrated ferromagnets

机译:立方体磁化的异常温度和场的行为   格子沮丧的铁磁体

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摘要

Thermodynamic properties of cubic Heisenberg ferromagnets with competingexchange interactions are considered near the frustration point where thecoefficient $D$ in the spin-wave spectrum $E_{\mathbf{k}}\sim D k^{2}$vanishes. Within the Dyson-Maleev formalism it is found that at lowtemperatures thermal fluctuations stabilize ferromagnetism by increasing thevalue of $D$. For not too strong frustration this leads to an unusual "concave"shape of the temperature dependence of magnetization, which is in agreementwith experimental data on the europium chalcogenides. Anomalous temperaturebehavior of magnetization is confirmed by Monte Carlo simulation. Strong fielddependence of magnetization (paraprocess) at finite temperature is found nearthe frustration point.
机译:带有竞争交换相互作用的立方海森堡铁磁体的热力学性质被认为是在挫折点附近,自旋波谱$ E _ {\ mathbf {k}} \ sim D k ^ {2} $中的系数$ D $消失。在Dyson-Maleev形式主义中,发现在低温下,热波动通过增加$ D $的值来稳定铁磁性。对于不太强烈的挫败感,这导致磁化的温度依赖性具有不寻常的“凹形”形状,这与关于硫族硫化物的实验数据一致。磁化的异常温度行为通过蒙特卡洛模拟得到证实。在受挫点附近发现了有限温度下强磁化(副过程)的场依赖性。

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