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光晶格中 p 轨道玻色子的手性轨道磁矩。

Chiral Orbital Magnetism of p-Orbital Bosons in Optical Lattices.

机构信息

Department of Applied Physics, School of Science, Xi'an Jiaotong University, Xi'an 710049, Shaanxi, China.

Shaanxi Province Key Laboratory of Quantum Information and Quantum Optoelectronic Devices, Xi'an Jiaotong University, Xi'an 710049, Shaanxi, China.

出版信息

Phys Rev Lett. 2018 Jul 6;121(1):015303. doi: 10.1103/PhysRevLett.121.015303.

Abstract

Chiral magnetism is a fascinating quantum phenomena that has been found in low-dimensional magnetic materials. It is not only interesting for understanding the concept of chirality, but also important for potential applications in spintronics. Past studies show that chiral magnets require both a lack of inversion symmetry and spin-orbit coupling to induce the Dzyaloshinskii-Moriya interaction. Here we report that the combination of inversion symmetry breaking and quantum degeneracy of orbital degrees of freedom will provide a new paradigm to achieve chiral orbital magnetism. By means of density matrix renormalization group calculation, we demonstrate that chiral orbital magnetism can be found when considering bosonic atoms loaded in the p band of an optical lattice in the Mott regime. The high tunability of our scheme is also illustrated through simply manipulating the inversion symmetry of the system for cold atom experimental conditions.

摘要

手性磁学是一种令人着迷的量子现象,已在低维磁性材料中被发现。它不仅对理解手性的概念很有趣,而且对自旋电子学的潜在应用也很重要。过去的研究表明,手性磁体需要同时缺乏反演对称性和自旋轨道耦合来诱导 Dzyaloshinskii-Moriya 相互作用。在这里,我们报告说,反转对称性破缺和轨道自由度的量子简并将提供一个新的范例来实现手性轨道磁学。通过密度矩阵重整化群计算,我们证明了当考虑玻色原子在莫特区的光学晶格的 p 带中被加载时,可以发现手性轨道磁学。我们的方案的高度可调性也通过简单地操纵系统的反演对称性来阐明,以适应冷原子实验条件。

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