{ "id": "cond-mat/0008259", "version": "v2", "published": "2000-08-17T20:40:28.000Z", "updated": "2000-08-22T18:18:08.000Z", "title": "Finite Temperature Magnetism in Fractional Quantum Hall Systems: Composite Fermion Hartree-Fock and Beyond", "authors": [ "Ganpathy Murthy" ], "comment": "10 pages, 8 eps figures. Two references added", "doi": "10.1088/0953-8984/12/50/315", "categories": [ "cond-mat.mes-hall" ], "abstract": "Using the Hamiltonian formulation of Composite Fermions developed recently, the temperature dependence of the spin polarization is computed for the translationally invariant fractional quantum Hall states at $\\nu=1/3$ and $\\nu=2/5$ in two steps. In the first step, the effect of particle-hole excitations on the spin polarization is computed in a Composite Fermion Hartree-Fock approximation. The computed magnetization for $\\nu=1/3$ lies above the experimental results for intermediate temperatures indicating the importance of long wavelength spin fluctuations which are not correctly treated in Hartree-Fock. In the second step, spin fluctuations beyond Hartree-Fock are included for $\\nu=1/3$ by mapping the problem on to the coarse-grained continuum quantum ferromagnet. The parameters of the effective continuum quantum ferromagnet description are extracted from the preceding Hartree-Fock analysis. After the inclusion of spin fluctuations in a large-N approach, the results for the finite-temperature spin polarization are in quite good agreement with the experiments.", "revisions": [ { "version": "v2", "updated": "2000-08-22T18:18:08.000Z" } ], "analyses": { "keywords": [ "fractional quantum hall systems", "composite fermion hartree-fock", "finite temperature magnetism", "fractional quantum hall states", "continuum quantum ferromagnet description" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 10, "language": "en", "license": "arXiv", "status": "editable" } } }