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首页> 外文期刊>Physical Review X >Disorder-Induced Transformation of the Energy Landscapes and Magnetization Dynamics in Two-Dimensional Ensembles of Dipole-Coupled Magnetic Nanoparticles
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Disorder-Induced Transformation of the Energy Landscapes and Magnetization Dynamics in Two-Dimensional Ensembles of Dipole-Coupled Magnetic Nanoparticles

机译:偶极耦合磁性纳米粒子二维集合中的能量景观和磁化动力学的紊乱诱导的变化

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The interaction-energy landscapes (ELs) and magnetization dynamics of two-dimensional ensembles of dipole-coupled magnetic nanoparticles are theoretically investigated. Extended nanostructures are modeled by considering nonoverlapping nanoparticles (NPs) in a square unit cell with periodic boundary conditions. The local minima and connecting transition states of the EL are determined systematically for representative NP arrangements having different degrees of disorder. The topology of the ergodic networks of stationary points is analyzed from both local and energy perspectives by using kinetic networks and disconnectivity graphs. We show that increasing the degree of disorder not only increases, most significantly, the number of local minima and transition states but also changes the shape of the EL in a very profound way. While slightly disordered ensembles correspond to good structure seekers, which are funneled towards the global minima, strongly disordered systems show very rough landscapes with multiple low-energy local minima separated by relatively large energy barriers. The consequences of this transition on the long-time Markovian dynamics of the nanostructures are quantified by calculating the field-free magnetic relaxation after saturation and after quenching. The simulations indicate that the relaxation of weakly disordered systems follows a slightly stretched exponential law, with a single characteristic timescale for a wide range of temperatures. In contrast, strongly disordered systems show a much more complicated relaxation dynamics involving multiple timescales, slowing down and trapping, which is reminiscent of spin glasses.
机译:理论上研究了二维偶联磁性纳米粒子的二维组合的相互作用景观(ELS)和磁化动态。通过在具有周期性边界条件的方形单元电池中考虑非覆盖纳米颗粒(NPS)来建模扩展的纳米结构。 EL的局部最小值和连接转换状态系统地确定具有不同无序程度的代表性NP布置。通过使用动力网络和断开图,通过局部和能量观点分析了静止点静态网络的拓扑。我们表明,增加紊乱程度不仅增加,最重要的是局部最小和过渡状态的数量,而且还以非常深刻的方式改变了EL的形状。虽然略微无序的整合对应于良好的结构寻求者,但朝​​向全球最小值漏斗,强烈无序的系统显示出非常粗糙的景观,其中具有相对大的能量屏障分离的多个低能量局部最小值。通过在饱和后和淬火之后计算无场磁松弛来量化该转变对纳米结构的长时间马尔可夫动力学的后果。该模拟表明,弱错乱系统的松弛遵循略微拉伸的指数律,具有各种温度的特征时间尺度。相比之下,强烈紊乱的系统显示出更复杂的松弛动态,涉及多个时间尺度,减速和捕获,这使得旋转玻璃。

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