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非磁性铁电体中的隐藏k空间磁电多极子

Hidden k-Space Magnetoelectric Multipoles in Nonmagnetic Ferroelectrics.

作者信息

Bhowal Sayantika, Collins Stephen P, Spaldin Nicola A

机构信息

Materials Theory, ETH Zurich, Wolfgang-Pauli-Strasse 27, 8093 Zurich, Switzerland.

Diamond Light Source Ltd, Diamond House, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, United Kingdom.

出版信息

Phys Rev Lett. 2022 Mar 18;128(11):116402. doi: 10.1103/PhysRevLett.128.116402.

Abstract

In condensed matter systems, the electronic degrees of freedom are often entangled to form complex composites, known as hidden orders, which give rise to unusual properties, while escaping detection in conventional experiments. Here we demonstrate the existence of hidden k-space magnetoelectric multipoles in nonmagnetic systems with broken space-inversion symmetry. These k-space magnetoelectric multipoles are reciprocal to the real-space charge dipoles associated with the broken inversion symmetry. Using the prototypical ferroelectric PbTiO_{3} as an example, we show that their origin is a spin asymmetry in momentum space resulting from the broken space inversion symmetry associated with the ferroelectric polarization. In PbTiO_{3}, the k-space spin asymmetry corresponds to a pure k-space magnetoelectric toroidal moment, which can be detected using magnetic Compton scattering, an established tool for probing magnetism in ferromagnets or ferrimagnets with a net spin polarization, which has not been exploited to date for nonmagnetic systems. In particular, the k-space magnetoelectric toroidal moment combined with the spin-orbit interaction manifest in an antisymmetric magnetic Compton profile that can be reversed using an electric field. Our work suggests an experimental route to directly measuring and tuning hidden k-space magnetoelectric multipoles via specially designed magnetic Compton scattering measurements.

摘要

在凝聚态系统中,电子自由度常常相互纠缠形成复杂的复合体,即所谓的隐藏序,它们会产生异常特性,同时在传统实验中难以被探测到。在此,我们展示了在具有空间反演对称性破缺的非磁性系统中隐藏的k空间磁电多极子的存在。这些k空间磁电多极子与因反演对称性破缺而产生的实空间电荷偶极子互为倒易。以典型的铁电体PbTiO₃为例,我们表明它们的起源是动量空间中的自旋不对称性,这是由与铁电极化相关的空间反演对称性破缺所导致的。在PbTiO₃中,k空间自旋不对称性对应于一个纯的k空间磁电环形矩,可利用磁康普顿散射进行探测,磁康普顿散射是一种用于探测具有净自旋极化的铁磁体或亚铁磁体中磁性的既定工具,迄今尚未用于非磁性系统。特别地,k空间磁电环形矩与自旋轨道相互作用相结合,表现为一种反对称磁康普顿轮廓,可通过电场进行反转。我们的工作提出了一条通过专门设计的磁康普顿散射测量来直接测量和调控隐藏的k空间磁电多极子的实验途径。

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