首页> 外文OA文献 >Sign problem free quantum Monte-Carlo study on thermodynamic properties and magnetic phase transitions in orbital-active itinerant ferromagnets
【2h】

Sign problem free quantum Monte-Carlo study on thermodynamic properties and magnetic phase transitions in orbital-active itinerant ferromagnets

机译:符号无问题量子monte-Carlo热力学性质研究   轨道活跃的巡回铁磁体中的磁相变和磁相变

代理获取
本网站仅为用户提供外文OA文献查询和代理获取服务,本网站没有原文。下单后我们将采用程序或人工为您竭诚获取高质量的原文,但由于OA文献来源多样且变更频繁,仍可能出现获取不到、文献不完整或与标题不符等情况,如果获取不到我们将提供退款服务。请知悉。

摘要

The microscopic mechanism of itinerant ferromagnetism is a long-standingproblem due to the lack of non-perturbative methods to handle strong magneticfluctuations of itinerant electrons. We have non-pertubatively studiedthermodynamic properties and magnetic phase transitions of a two-dimensionalmulti-orbital Hubbard model exhibiting ferromagnetic ground states. QuantumMonte-Carlo simulations are employed, which are proved in a wide density regionfree of the sign problem usually suffered by simulations for fermions. BothHund's coupling and electron itinerancy are essential for establishing theferromagnetic coherence. No local magnetic moments exist in the system as apriori, nevertheless, the spin channel remains incoherent showing theCurie-Weiss type spin magnetic susceptibility down to very low temperatures atwhich the charge channel is already coherent exhibiting a weaklytemperature-dependent compressibility. For the SU(2) invariant systems, thespin susceptibility further grows exponentially as approaching zero temperaturein two dimensions. In the paramagnetic phase close to the Curie temperature,the momentum space Fermi distributions exhibit strong resemblance to those inthe fully polarized state. The long-range ferromagnetic ordering appears whenthe symmetry is reduced to the Ising class, and the Curie temperature isaccurately determined. These simulations provide helpful guidance to searchingfor novel ferromagnetic materials in both strongly correlated $d$-orbitaltransition metal oxide layers and the $p$-orbital ultra-cold atom opticallattice systems.
机译:流动铁磁性的微观机制是一个长期存在的问题,原因是缺乏处理流动电子强磁波动的非扰动方法。我们已经非渗透性地研究了呈现铁磁基态的二维多轨道哈伯德模型的热力学性质和磁相变。使用了QuantumMonte-Carlo模拟,该模拟在宽密度区域得到证明,而没有费米子模拟通常遇到的符号问题。洪德的耦合和电子迭代对于建立铁磁相干性至关重要。系统中不存在先验的局部磁矩,尽管如此,自旋通道仍保持非相干性,表明Curie-Weiss型自旋磁化率低至非常低的温度,此时电荷通道已经相干,表现出与温度无关的弱压缩性。对于SU(2)不变系统,旋转敏感性在二维接近零温度时进一步呈指数增长。在接近居里温度的顺磁相中,动量空间费米分布与全极化状态下的动量空间很相似。当对称性降低到Ising类并准确确定居里温度时,就会出现远距离铁磁有序。这些模拟为在强相关的$ d $轨道过渡金属氧化物层和$ p $轨道超冷原子光学晶格系统中寻找新型铁磁材料提供了有用的指导。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
代理获取

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号