paper

Hilbert space structure of the low energy sector of U(N) quantum Hall ferromagnets and their classical limit

arXiv:1904.06932 · doi:10.3390/sym14050872

Abstract

Using the Lieb-Mattis ordering theorem of electronic energy levels, we identify the Hilbert space of the low energy sector of U() quantum Hall/Heisenberg ferromagnets at filling factor for Landau/lattice sites with the carrier space of irreducible representations of U() described by rectangular Young tableaux of rows and columns, and associated with Grassmannian phase spaces U()/U()U(). We embed this -component fermion mixture in Fock space through a Schwinger-Jordan (boson and fermion) representation of U()-spin operators. We provide different realizations of basis vectors using Young diagrams, Gelfand-Tsetlin patterns and Fock states (for an electron/flux occupation number in the fermionic/bosonic representation). U()-spin operator matrix elements in the Gelfand-Tsetlin basis are explicitly given. Coherent state excitations above the ground state are computed and labeled by complex matrix points on the Grassmannian phase space. They adopt the form of a U() displaced/rotated highest-weight vector, or a multinomial Bose-Einstein condensate in the flux occupation number representation. Replacing U()-spin operators by their expectation values in a Grassmannian coherent state allows for a semi-classical treatment of the low energy (long wavelength) U()-spin-wave coherent excitations (skyrmions) of U() quantum Hall ferromagnets in terms of Grasmannian nonlinear sigma models.

24 pages, no figures. Version to appear in the Special Issue "Topological Spin Textures: From Fundamentals to Applications" of Symmetry

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