We present analytic formulas for the ground state energy of the two-dimensional (2D) anyon gas in the quantum limit of a perpendicular magnetic field (Landau level filling factor ν_L\le 1). These formulas, for the cases without and with Coulomb interaction, are obtained by applying the harmonic potential regularization for vanishing confinement to the harmonically confined Coulomb anyon gas as in our previous paper for the case without magnetic field. For the case without Coulomb interaction our analytic expression is exact. It contains a contribution deriving from the anyon gauge field (characterizing the fractional statistics by the anyon parameter ν) and depends on νand ν_L. For the case with Coulomb interaction we introduce a function, depending on ν, ν_L and the density parameter r_s, which is determined by fitting to the interpolation formula of Fano and Ortolani in the fractional quantum Hall regime for spin-polarized fermions in conjunction with results of Yoshioka for the ground state energy of the 2D Coulomb boson gas in high magnetic fields. With their dependence on ν, our formulas apply not only to fermions (ν=1) but quite generally to anyons (0\le ν\le 1).
Local spectroscopy of anyons bound to charge traps
Princeton University（普林斯顿大学）；University of Leeds（利兹大学）；Flatiron Institute（平顿研究所）；Washington University in St. Louis（圣路易斯华盛顿大学）；National Institute for Materials Science（国立材料研究所）；University of Cambridge（剑桥大学）；University of California at Berkeley（加州大学伯克利分校）
