Measuring the Chern number of Hofstadter bands with ultracold bosonic atoms

• Published in: Nature physics Vol. 11; no. 2; pp. 162 - 166
• Main Authors: Aidelsburger, M., Lohse, M., Schweizer, C., Atala, M., Barreiro, J. T., Nascimbène, S., Cooper, N. R., Bloch, I., Goldman, N.
• Format: Journal Article
• Language: English
• Published: London Nature Publishing Group UK 01.02.2015; Nature Publishing Group
• Subjects: 639/766/119/2794; 639/766/36/1125; 639/766/483/3926; Atomic; Atomic properties; Bands; Classical and Continuum Physics; Clouds; Complex Systems; Condensed Matter Physics; Deflection; Electromagnetism; Electronic systems; Ferromagnetism; Gages; Invariants; letter; Mathematical and Computational Physics; Molecular; Optical and Plasma Physics; Physics; Quantum Hall effect; Superlattices; Theoretical; Topology; Transport; Ultracold atoms
• ISSN: 1745-2473; 1745-2481
• DOI: 10.1038/nphys3171

Chern numbers characterize the quantum Hall effect conductance—non-zero values are associated with topological phases. Previously only spotted in electronic systems, they have now been measured in ultracold atoms subject to artificial gauge fields. Sixty years ago, Karplus and Luttinger pointed out that quantum particles moving on a lattice could acquire an anomalous transverse velocity in response to a force, providing an explanation for the unusual Hall effect in ferromagnetic metals 1 . A striking manifestation of this transverse transport was then revealed in the quantum Hall effect 2 where the plateaux depicted by the Hall conductivity were attributed to a topological invariant characterizing the Bloch bands: the Chern number 3 . Until now, topological transport associated with non-zero Chern numbers has only been observed in electronic systems 2 , 4 , 5 . Here we use the transverse deflection of an atomic cloud in response to an optical gradient to measure the Chern number of artificially generated Hofstadter bands 6 . These topological bands are very flat and thus constitute good candidates for the realization of fractional Chern insulators 7 . Combining these deflection measurements with the determination of the band populations, we obtain an experimental value for the Chern number of the lowest band ν exp = 0.99(5). This first Chern-number measurement in a non-electronic system is facilitated by an all-optical artificial gauge field scheme, generating uniform flux in optical superlattices.