2017/10/02 by Mitali Banerjee, Moty Heiblum, Vladimir Umansky +3 · 3 citations
Physics and Astronomy · #cond-mat.mes-hall
paper · pdf · doi:10.1038/s41586-018-0184-1
16 pages, 16 figures
arxiv created 2017/10/02 · arxiv updated 2018/09/05
Topological states of matter are characterized by topological invariant, which are physical quantities whose values are quantized and do not depend on details of the measured system. Of these, the easiest to probe in experiments is the electrical Hall conductance, which is expressed in units of e2/h (e the electron charge, h the Planck's constant). In the fractional quantum Hall effect (FQHE), fractional quantized values of the electrical Hall conductance attest to topologically ordered states, which are states that carry quasi particles with fractional charge and anyonic statistics. Another topological invariant, which is much harder to measure, is the thermal Hall conductance, expressed in units of κ0T=(π2kB2/3h)T (kB the Boltzmann constant, T the temperature). For the quantized thermal Hall conductance, a fractional value attests that the probed state of matter is non-abelian. Quasi particles in non-abelian states lead to a ground state degeneracy and perform topological unitary transformations among ground states when braided. As such, they may be useful for topological quantum computation. In this paper, we report our measurements of the thermal Hall conductance for several quantum Hall states in the first excited Landau level. Remarkably, we find the thermal Hall conductance of the ν=5/2 state to be fractional, and to equal 2.5κ0T