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Field induced magnetic ordering transition in Kondo insulators

机译:近藤绝缘子的磁场感应磁有序跃迁

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We study the 2D Kondo insulators in a uniform magnetic field using quantum Monte Carlo simulations of the particle-hole symmetric Kondo lattice model and a mean field analysis of the Periodic Anderson model. We find that the field induces a transition to an insulating, antiferromagnetically ordered phase with staggered moment in the plane perpendicular to the field. For fields in excess of the quasi-particle gap, corresponding to a metal in a simple band picture of the periodic Anderson model, we find that the metallic phase is unstable towards the spin density wave type ordering for any finite value of the interaction strength. This can be understood as a consequence of the perfect nesting of the particle and hole Fermi surfaces that emerge as the field closes the gap. We propose a phase diagram and investigate the quasi-particle and charge excitations in the magnetic field. We find good agreement between the mean-field and quantum Monte Carlo results.
机译:我们使用粒子孔对称近藤晶格模型的量子蒙特卡洛模拟和周期安德森模型的平均场分析,研究了均匀磁场中的二维近藤绝缘子。我们发现,该场在垂直于该场的平面中以交错的矩感应出一个过渡到绝缘的反铁磁有序相。对于超出准粒子间隙的场(对应于周期性Anderson模型的简单带图中的金属),我们发现对于任何有限的相互作用强度值,金属相都对自旋密度波类型不稳定。这可以理解为由于电场闭合间隙而出现的粒子和空穴费米表面的完美嵌套的结果。我们提出了一个相图,并研究了磁场中的准粒子和电荷激发。我们发现平均场和量子蒙特卡洛结果之间有很好的一致性。

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