The nature of composite fermions and the role of particle hole symmetry: A microscopic account
arXiv:1604.03911 · doi:10.1103/PhysRevB.93.235152
Abstract
Motivated by the issue of particle-hole symmetry for the composite fermion Fermi sea at the half filled Landau level, Dam T. Son has made an intriguing proposal [Phys. Rev. X {\bf 5}, 031027 (2015)] that composite fermions are Dirac particles. We ask what features of the Dirac-composite fermion theory and its various consequences may be reconciled with the well established microscopic theory of the fractional quantum Hall effect and the 1/2 state, which is based on {\em non-relativistic} composite fermions. Starting from the microscopic theory, we derive the assertion of Son that the particle-hole transformation of electrons at filling factor corresponds to an effective time reversal transformation (i.e. ) for composite fermions, and discuss how this connects to the absence of backscattering in the presence of a particle-hole symmetric disorder. By considering bare holes in various composite-fermion levels (analogs of electronic Landau levels) we determine the level spacing and find it to be very nearly independent of the level index, consistent with a parabolic dispersion for the underlying composite fermions. Finally, we address the compatibility of the Chern-Simons theory with the lowest Landau level constraint, and find that the wave functions of the mean-field Chern-Simons theory, as well as a class of topologically similar wave functions, are surprisingly accurate when projected into the lowest Landau level. These considerations lead us to introduce a "normal form" for the unprojected wave functions of the states that correctly capture the topological properties even without lowest Landau level projection.
arXiv comment17 pages, 3 figures, published version
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