论文标题
WSE2单层中的应变可调浆果曲率偶极子,轨道磁化和非线性霍尔效应
Strain Tunable Berry Curvature Dipole, Orbital Magnetization and Nonlinear Hall Effect in WSe2 Monolayer
论文作者
论文摘要
电子拓扑通常与浆果曲率有关,浆果曲率可以诱导时间反转对称性破坏系统中的异常霍尔效应。固有的单层过渡金属二核苷具有两个不需要的k和k'valleys,具有相反符号的浆果曲率,因此在该系统中消失了异常的霍尔效应。在这里,我们报告了单层WSE2中单轴菌株中的单轴菌株破坏C3V对称性的单层WSE2中浆果曲率不对称分布的实验实现。结果,尽管浆果曲率本身在K和K'Valleys中仍然相反,但两个山谷将同样贡献非零浆果曲率偶极子。应用电场后,出现的浆果曲率偶极子将导致平面外轨道磁化强度,这进一步诱导了异常的霍尔效应,其线性响应对E^2(称为非线性霍尔效应)。我们显示了单层WSE2中非线性霍尔效应的应变调制传输特性,并通过门控中等孔掺杂。第二谐波大厅信号显示出对电场的二次依赖性,并且每个电流密度的相应轨道磁化强度可以达到60。与常规的Rashba-Edelstein效应与平面自旋极化相比,这种电流诱导的轨道磁化强度沿着平面的方向沿底层式启动,因此具有良好的启发性启动。
The electronic topology is generally related to the Berry curvature, which can induce the anomalous Hall effect in time-reversal symmetry breaking systems. Intrinsic monolayer transition metal dichalcogenides possesses two nonequivalent K and K' valleys, having Berry curvatures with opposite signs, and thus vanishing anomalous Hall effect in this system. Here we report the experimental realization of asymmetrical distribution of Berry curvature in a single valley in monolayer WSe2 through applying uniaxial strain to break C3v symmetry. As a result, although the Berry curvature itself is still opposite in K and K' valleys, the two valleys would contribute equally to nonzero Berry curvature dipole. Upon applying electric field, the emergent Berry curvature dipole would lead to an out-of-plane orbital magnetization, which further induces an anomalous Hall effect with a linear response to E^2, known as nonlinear Hall effect. We show the strain modulated transport properties of nonlinear Hall effect in monolayer WSe2 with moderate hole-doping by gating. The second-harmonic Hall signals show quadratic dependence on electric field, and the corresponding orbital magnetization per current density can reach as large as 60. In contrast to the conventional Rashba-Edelstein effect with in-plane spin polarization, such current-induced orbital magnetization is along the out-of-plane direction, thus promising for high-efficient electrical switching of perpendicular magnetization.