Abstract

We propose an interferometric method to measure Z2 topological invariants of time-reversal invariant topological insulators realized with optical lattices in two and three dimensions. We suggest two schemes which both rely on a combination of Bloch oscillations with Ramsey interferometry and can be implemented using standard tools of atomic physics. In contrast to topological Zak phase and Chern number, defined for individual 1D and 2D Bloch bands, the formulation of the Z2 invariant involves at least two Bloch bands related by time- reversal symmetry which one has keep track of in measurements. In one of our schemes this can be achieved by the measurement of Wilson loops, which are non-Abelian generalizations of Zak phases. The winding of their eigenvalues is related to the Z2 invariant. We thereby demonstrate that Wilson loops are not just theoretical concepts but can be measured experimentally. For the second scheme we introduce a generalization of time-reversal polarization which is continuous throughout the Brillouin zone. We show that its winding over half the Brillouin zone yields the Z2 invariant. To measure this winding, our protocol only requires Bloch oscillations within a single band, supplemented by coherent transitions to a second band which can be realized by lattice-shaking.

Highlights

  • It has been understood almost since its discovery in 1980 that the quantum Hall effect [1] emerges from the nontrivial topology of Landau levels [2]

  • We proceed by giving the theoretical derivation of the phases to be measured; we show their relation to the Z2 invariant and present a mathematical formulation of continuous time-reversal polarization

  • Summarizing, we have shown that the Z2-invariant classifying time-reversal invariant topological insulators can be measured using a combination of Bloch oscillations and Ramsey interferometry

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Summary

INTRODUCTION

It has been understood almost since its discovery in 1980 that the quantum Hall effect [1] emerges from the nontrivial topology of Landau levels [2]. Berry phases and corresponding topological invariants were directly measured in a cold atomic system in an optical lattice [16] allowing a direct experimental investigation of the topology of Bloch band wave functions. A different approach to measure Chern numbers makes use of the Streda formula, relating them to the change in atomic density when a finite magnetic field is switched on [46,47] Extensions of this method for detection of Z2 topological phases were suggested [30,31], they only work when the Chern numbers for individual spins are well defined (which is generally not the case [48]). V we conclude and give an outlook on how our scheme can be applied to 3D topological insulators

INTERFEROMETRIC MEASUREMENT OF THE Z2 INVARIANT
Zak phases
Chern numbers and Zak phases
Z2 invariant and time-reversal polarization
Discontinuity of time-reversal polarization
The twist scheme
Z2 invariant and Wilson loops
Wilson loops
Relation to Z2 invariant
The Wilson loop scheme
Relation between Wilson loops and TRP
TWIST SCHEME
Interferometric sequence
Band switchings
Sequence
Dynamical-phase-free sequence
Experimental realization and limitations
Formal definition and calculation of cTRP
Definition of cTRP
Discretized version of continuous time-reversal polarization
Example
WILSON LOOP SCHEME
TR Wilson loops and their phases
Total Zak phase
SUMMARY AND OUTLOOK
The 3D case
Full Text
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