arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2602.08844cond-mat.mes-hallhep-th
收藏

非常规磁电导率和电化学响应来自 Berry 曳度的偶极子源

Unconventional magnetoelectric conductivity and electrochemical response from dipole-like sources of Berry curvature

Shiv Nadar Institution of Eminence (SNIoE)(Shiv Nadar卓越机构)

Ipsita Mandal

AI总结:

研究通过半经典玻尔兹曼方法,分析了三种半金属体系中 Berry 曳度偶极子源对磁电导率和电化学响应的影响。

摘要:

我们计算了三维节点环半金属(漩涡节点环和 PT 对称节点环)和三带霍普夫半金属的纵向磁电导率(σ zz)和非线性电化学响应(ECR),应用半经典玻尔兹曼形式法。虽然前者的节点曲线被取在k z = 0平面,后者的节点点在其 Berry 曳度(BC)分布中具有偶极子,其偶极子轴沿k z轴对齐。所有这些系统都是拓扑的,并且在它们的带具有消失的陈数方面统一。线性响应σ zz是从当系统受到沿各向异性轴(即z轴)的平行电场和磁场作用时的精确解获得的。非线性部分涉及三阶张量,代表二阶响应系数,将电流与化学势梯度和外部电场的联合效应联系起来。我们分析了漩涡节点环和霍普夫半金属响应的相似性,这可以追溯到它们的 BC 场中偶极子源。

英文摘要:

We investigate the longitudinal magnetoelectric conductivity and nonlinear electrochemical response (ECR) of three-dimensional nodal-ring semimetals, including vortex nodal-rings (VNRs) and $\mathcal{PT}$-symmetric nodal-rings (PTNRs), together with three-band Hopf semimetals (HSMs), using the semiclassical Boltzmann formalism. The nodal-rings of the VNRs and PTNRs lie in the $k_z=0$ plane, whereas the nodal points of HSMs host isolated Berry-curvature (BC) dipoles with axes along the $k_z$ direction. In VNRs, such dipoles may be viewed as forming a continuous distribution along the nodal-ring, connecting the two classes of systems. For collinear electric and magnetic ($\mathcal{B}$) fields along the anisotropy axis $\boldsymbol {\hat{z}}$, the linear response is computed exactly and displays odd powers of $B_z$ for a single ring or node. For a two-node HSM with oppositely-oriented BC-dipole axes, these odd terms cancel in the sum. We analyse the nonlinear ECR, described by third-rank response tensors that relate the current to the combined action of an electric field and a chemical-potential gradient. The surviving tensor components are determined by the tilt direction of the bandstructure, and we obtain explicit results for simultaneous in-plane and axial tilts. A comparison of the three systems reveals a close correspondence between the responses of VNRs and HSMs, while PTNRs behave qualitatively differently. We attribute these similarities and differences to the topology of the BC field, namely dipole-like sources in VNRs and HSMs versus the ring-confined BC structure of PTNRs.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑