Chern Numbers Hiding in Time of Flight Images

Abstract

We present a novel technique for detecting topological invariants ‐ Chern numbers ‐ from time-of-flight images of ultra-cold atoms. We show that the Chern numbers of integer quantum Hall states of lattice fermions leave their fingerprints as oscillations in the atoms’ momentum distribution. The number of oscillations within the lowest Brillouin zone is simply equal to the Chern number. The ubiquitous signature is strikingly enhanced for anisotropic hopping, where the momentum distribution assumes a sinusoidal form with period determined by the Chern number. Thus, an everyday observable in cold atom experiments can serve as a useful tool to characterize and visualize quantum states with non-trivial topology. Topological insulators (TI) and superfluids are many-body quantum systems with energy gaps in the bulk but topologically protected, gapless excitations on the boundary [1, 2]. Each class of topological phases is characterized by a topological invariant which can be either an integer or a binary quantity. For example, the integer quantum Hall insulators [3] are distinguished from other two-dimensional insulators with the same symmetry by the Chern number, an integer that capture the global properties of all occupied bands [4]. The Chern number coincides with the number of chiral edge modes, and the Hall conductance in units of the conductance quantum. A central problem in exploring new forms of topological matter is how to extract the topological invariants from experiments, and unambiguously determine the topological phase. Experiments with ultracold atoms has brought us opportunities to creating topological phases of matter in parameter regimes unreachable in solids. In addition to band-structure engineering using optical lattices and tuning the atom-atom interaction by Feshbach resonance, artificial magnetic fields for neutral atoms have been produced by either rotation [5] or atom-laser coupling [6, 7], making way to realizing quantum Hall states of cold atoms [8]. Moreover, non-Abelian synthetic gauge fields [7, 9] and spin-orbit coupling [10] have been demonstrated. These developments motivated theories on properties of ultracold topological matter, e.g., the fractional quantum Hall effect of interacting bosons [5, 11, 12], the quantum spin Hall effect of fermions [9], and the quantum anomalous Hall states ofp-orbital fermions [13]. While cold atom systems offer new detection techniques and great tunability, it is challenging to measure the topological invariants directly. Measurements of local density of states (of the edge states) or mass transport are marred with complexity in contrast to solid state systems. Thus, creative methods have to be invented. For example, Ref. [8] proposed to extract the quantized Hall conductance from the derivatives