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arXiv 2201.03883cond-mat.stat-mechcond-mat.mtrl-sci
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具有时空变化的高斯随机外磁场对 Ising 自旋-1/2 三层方形亚铁磁体补偿效应的影响

Effect of a Gaussian random external magnetic field with spatio temporal variation on compensation in Ising spin-1/2 trilayered square ferrimagnets

Soham Chandra

AI总结:

本研究利用 Metropolis Monte Carlo 模拟探讨了时空变化的高斯随机外磁场对三层 spin-1/2 Ising 亚铁磁体补偿现象的影响,发现随机场会导致补偿点偏移甚至消失,并揭示了无补偿相区域面积随外场标准差变化的标度关系。

摘要:

本研究进行了广泛的 Metropolis Monte Carlo 模拟,以探讨由具有特定时空变化的外部高斯随机磁场驱动的、具有方形单分子层的三层 spin-1/2 Ising 亚铁磁体的稳态磁性和热力学行为。这类亚铁磁薄膜系统表现出补偿现象,因此是多种技术应用的潜在候选者。这里,两种不同的理论原子 A 和 B 构成了 ABA 和 AAB 两种构型,其中同类原子(A-A 和 B-B)发生铁磁相互作用,不同类原子(A-B)发生反铁磁相互作用。根据时空变化的高斯随机场强度不同,补偿点和临界点发生偏移,且稳态磁行为在不同类型的亚铁磁行为之间发生转变。对于其他控制参数的特定选择,当磁场标准差超过有限阈值后,补偿现象甚至会消失。因此,在两种构型的 Hamiltonian 参数空间中,无补偿的亚铁磁相区域出现在无场情况下的有补偿相区域内。这些区域的面积随着外场标准差 σ 的增加而增大,遵循标度关系:f(σ, A(σ))=σ^{-b}A(σ),其中 b_{ABA}=1.913±0.137,b_{AAB}=1.625±0.066。这些指数值在统计区间内与均匀随机磁场下获得的值相匹配。

英文摘要:

In this work, an extensive Metropolis Monte Carlo simulation is performed to investigate the steady-state magnetic and thermodynamic behaviour of a trilayered spin-1/2 Ising ferrimagnet with square monolayers, driven by external Gaussian random magnetic field with certain spatio-temporal variations. Such thin ferrimagnetic systems exhibit compensation phenomenon and thus are potentially interesting candidates for several technological applications. Here, two distinct theoretical atoms, A and B, make up the ABA and AAB types of configurations in which the like atoms (A-A and B-B) ferromagnetically interact and the unlike atoms (A-B) interact antiferromagnetically. Depending upon the strength of the spatio-temporally varying Gaussian random field, the compensation and critical points shift and steady-state magnetic behaviours change between the different distinct types of ferrimagnetic behaviours. The compensation phenomenon even vanishes after crossing a finite threshold of the standard deviation of the magnetic field for particular choices of the other controlling parameters. Consequently, in the Hamiltonian parameter space of both configurations, islands of ferrimagnetic phase without compensation appear within the phase area with compensation of field-free case. The areas of such islands grow with an increasing standard deviation of the external field, $σ$, obeying the scaling relation: $f(σ, A(σ))=σ^{-b}A(σ)$ with $b_{ABA}=1.913\pm 0.137$ and $b_{AAB}=1.625\pm 0.066$ . These values of exponents match within the statistical interval with those obtained with the uniform random magnetic field.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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