Li, X.Zhang, FanMacDonald, A. H.2016-09-232016-09-232016-01-152016-01-150031-9007http://hdl.handle.net/10735.1/5065The (111) surface of SnTe hosts one isotropic Γ-centered and three degenerate anisotropic M-centered Dirac surface states. We predict that a nematic phase with spontaneously broken C₃ symmetry will occur in the presence of a perpendicular magnetic field when the N=0 M Landau levels are 1/3 or 2/3 filled. The nematic state phase boundary is controlled by a competition between intravalley Coulomb interactions that favor a valley-polarized state and weaker intervalley scattering processes that increase in relative strength with magnetic field. An in-plane Zeeman field alters the phase diagram by lifting the threefold M Landau-level degeneracy, yielding a ground state energy with 2π/3 periodicity as a function of Zeeman-field orientation angle.en©2016 American Physical SocietySymmetry (Physics)Dirac equationTelluridesCoulomb functionsZeeman effectSU(3) Quantum Hall Ferromagnetism in SnTeArticleLi, X., F. Zhang, and A. H. MacDonald. 2016. "SU(3) quantum hall ferromagnetism in SnTe." Physical Review Letters 116(2), doi:10.1103/PhysRevLett.116.026803.1162