Fractional Quantum Anomalous Hall Effect in Multilayer Graphene
ORAL
Abstract
The fractional quantum anomalous Hall effect (FQAHE)1, the analog of the fractional quantum Hall effect at zero magnetic field, is predicted to exist in topological flat bands under spontaneous time-reversal-symmetry breaking2-5. The demonstration of FQAHE could lead to non-Abelian anyons which form the basis of topological quantum computation6-8. So far, FQAHE has been observed only in twisted MoTe2 (t-MoTe2) at moiré filling factor v > 1/29-12. Graphene-based moiré superlattices are believed to host FQAHE with the potential advantage of material quality and electron mobility. In this talk, I will report the observation of integer and fractional QAH effects in a rhombohedral pentalayer graphene/hBN moiré superlattice. At zero magnetic field, we observed plateaus of quantized Hall resistance Rxy = h/(ve2) at moiré filling factors v = 1, 2/3, 3/5, 4/7, 4/9, 3/7 and 2/5. In addition, the phase transitions from composite Fermi liquid and FQAH states to other correlated states will also be discussed. The rich family of FQAH states in our graphene-based moiré superlattice provides an ideal platform for exploring charge fractionalization and (non-Abelian) anyonic braiding at zero magnetic field13-18.
*L.J. acknowledges support from a Sloan Fellowship. Work by T.H., J.Y. and J.S. was supported by NSF grant no. DMR- 2225925. The device fabrication of this work was supported by the STC Center for Integrated Quantum Materials, NSF grant no. DMR-1231319 and was carried out at the Harvard Center for Nanoscale Systems and MIT.Nano. Part of the device fabrication was supported by USD(R&E) under contract no. FA8702-15-D-0001. K.W. and T.T. acknowledge support from the JSPS KAKENHI (Grant Numbers 20H00354, 21H05233 and 23H02052) and World Premier International Research Center Initiative (WPI), MEXT, Japan. L.F. was supported by the STC Center for Integrated Quantum Materials (CIQM) under NSF award no. DMR-1231319.