论文标题
伪随方式杂质模型以均衡:主方程张量网络方法
Pseudogap Anderson impurity model out of equilibrium: A master equation tensor network approach
论文作者
论文摘要
我们研究了具有幂律伪群在状态的密度的单突击模型的平衡和非平衡性能。在平衡中,已知该模型显示从广义近代到局部力矩相的量子相变。在目前的工作中,我们关注这些阶段以外的均衡,即在偏置电压的影响下。在辅助主方程方法与基于矩阵乘积状态(MPS)方案的结合中,我们能够直接解决当前携带稳态的问题。从平衡情况开始,我们首先通过与MPS对系统的基态光谱特性进行直接数值评估来证实我们的结果。在这里,通过推断自能量的幂律指数来定位相边界的方案产生了非常良好的一致性,与数值重新归一化组获得的先前结果。然后,我们的非平衡研究作为应用偏置电压的函数,然后在相边界的两侧进行两个点。在Kondo制度中,光谱函数中的共振是偏置电压增加的函数。相反,局部力矩机制在化学势位置附近的光谱中显示出倾角。在相应的自能量中观察到类似的特征。 Kondo拆分峰值大约遵守幂律行为,其指数仅略微依赖于电压。最后,近野制度中的差分电导率显示出有限电压下的最大值,但是高度低于精度水平。
We study equilibrium and nonequilibrium properties of the single-impurity Anderson model with a power-law pseudogap in the density of states. In equilibrium, the model is known to display a quantum phase transition from a generalized Kondo to a local moment phase. In the present work, we focus on the extension of these phases beyond equilibrium, i.e. under the influence of a bias voltage. Within the auxiliary master equation approach combined with a scheme based on matrix product states (MPS) we are able to directly address the current-carrying steady state. Starting with the equilibrium situation, we first corroborate our results by comparing with a direct numerical evaluation of ground state spectral properties of the system by MPS. Here, a scheme to locate the phase boundary by extrapolating the power-law exponent of the self energy produces a very good agreement with previous results obtained by the numerical renormalization group. Our nonequilibrium study as a function of the applied bias voltage is then carried out for two points on either side of the phase boundary. In the Kondo regime the resonance in the spectral function is splitted as a function of the increasing bias voltage. The local moment regime, instead, displays a dip in the spectrum near the position of the chemical potentials. Similar features are observed in the corresponding self energies. The Kondo split peaks approximately obey a power-law behavior as a function of frequency, whose exponents depend only slightly on voltage. Finally, the differential conductance in the Kondo regime shows a peculiar maximum at finite voltages, whose height, however, is below the accuracy level.