A New Approach to Transport Coefficients in the Quantum Spin Hall Effect
Giovanna Marcelli, Gianluca Panati, Stefan Teufel
Abstract
Abstract We investigate some foundational issues in the quantum theory of spin transport, in the general case when the unperturbed Hamiltonian operator $$H_0$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>H</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:math> does not commute with the spin operator in view of Rashba interactions, as in the typical models for the quantum spin Hall effect. A gapped periodic one-particle Hamiltonian $$H_0$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>H</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:math> is perturbed by adding a constant electric field of intensity $$\varepsilon \ll 1$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>ε</mml:mi><mml:mo>≪</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:math> in the j -th direction, and the linear response in terms of a S -current in the i -th direction is computed, where S is a generalized spin operator. We derive a general formula for the spin conductivity that covers both the choice of the conventional and of the proper spin current operator. We investigate the independence of the spin conductivity from the choice of the fundamental cell ( unit cell consistency ), and we isolate a subclass of discrete periodic models where the conventional and the proper S -conductivity agree, thus showing that the controversy about the choice of the spin current operator is immaterial as far as models in this class are concerned. As a consequence of the general theory, we obtain that whenever the spin is (almost) conserved, the spin conductivity is (approximately) equal to the spin-Chern number. The method relies on the characterization of a non-equilibrium almost-stationary state (NEASS), which well approximates the physical state of the system (in the sense of space-adiabatic perturbation theory) and allows moreover to compute the response of the adiabatic S -current as the trace per unit volume of the S -current operator times the NEASS. This technique can be applied in a general framework, which includes both discrete and continuum models.