76 research outputs found

    Resonant Enhancement of Inelastic Light Scattering in the Fractional Quantum Hall Regime at ν=1/3\nu=1/3

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    Strong resonant enhancements of inelastic light scattering from the long wavelength inter-Landau level magnetoplasmon and the intra-Landau level spin wave excitations are seen for the fractional quantum Hall state at ν=1/3\nu = 1/3. The energies of the sharp peaks (FWHM 0.2meV\lesssim 0.2meV) in the profiles of resonant enhancement of inelastic light scattering intensities coincide with the energies of photoluminescence bands assigned to negatively charged exciton recombination. To interpret the observed enhancement profiles, we propose three-step light scattering mechanisms in which the intermediate resonant transitions are to states with charged excitonic excitations.Comment: 5 pages, 5 figure

    Splitting of Long-Wavelength Modes of the Fractional Quantum Hall Liquid at ν=1/3\nu=1/3

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    Resonant inelastic light scattering experiments at ν=1/3\nu=1/3 reveal a novel splitting of the long wavelength modes in the low energy spectrum of quasiparticle excitations in the charge degree of freedom. We find a single peak at small wavevectors that splits into two distinct modes at larger wavevectors. The evidence of well-defined dispersive behavior at small wavevectors indicates a coherence of the quantum fluid in the micron length scale. We evaluate interpretations of long wavelength modes of the electron liquid.Comment: 4 pages, 4 figure

    Spin texture and magnetoroton excitations at nu=1/3

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    Neutral spin texture (ST) excitations at nu=1/3 are directly observed for the first time by resonant inelastic light scattering. They are determined to involve two simultaneous spin flips. At low magnetic fields, the ST energy is below that of the magnetoroton minimum. With increasing in-plane magnetic field these mode energies cross at a critical ratio of the Zeeman and Coulomb energies of eta(c)=0.020 +/- 0.001. Surprisingly, the intensity of the ST mode grows with temperature in the range in which the magnetoroton modes collapse. The temperature dependence is interpreted in terms of a competition between coexisting phases supporting different excitations. We consider the role of the ST excitations in activated transport at nu=1/3

    Transition from Free to Interacting Composite Fermions away from ν\nu=1/3

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    Spin excitations from a partially populated composite fermion level are studied above and below ν=1/3\nu=1/3. In the range 2/7<ν<2/52/7<\nu<2/5 the experiments uncover significant departures from the non-interacting composite fermion picture that demonstrate the increasing impact of interactions as quasiparticle Landau levels are filled. The observed onset of a transition from free to interacting composite fermions could be linked to condensation into the higher order states suggested by transport experiments and numerical evaluations performed in the same filling factor range.Comment: 4 pages, 5 figures, to appear in PR

    Spin excitations in the Fractional Quantum Hall regime at ν1/3\nu\lesssim1/3

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    We report inelastic light scattering experiments in the fractional quantum Hall regime at filling factors ν1/3\nu\lesssim1/3. A spin mode is observed below the Zeeman energy. The filling factor dependence of the mode energy is consistent with its assignment to spin flip excitations of composite fermions with four attached flux quanta (ϕ\phi=4). Our findings reveal a composite fermion Landau level structure in the ϕ\phi=4 sequence.Comment: 7 pages, 4 figures, EP2DS-16 conference, to appear in Physica

    Gauge Theory of Composite Fermions: Particle-Flux Separation in Quantum Hall Systems

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    Fractionalization phenomenon of electrons in quantum Hall states is studied in terms of U(1) gauge theory. We focus on the Chern-Simons(CS) fermion description of the quantum Hall effect(QHE) at the filling factor ν=p/(2pq±1)\nu=p/(2pq\pm 1), and show that the successful composite-fermions(CF) theory of Jain acquires a solid theoretical basis, which we call particle-flux separation(PFS). PFS can be studied efficiently by a gauge theory and characterized as a deconfinement phenomenon in the corresponding gauge dynamics. The PFS takes place at low temperatures, TTPFST \leq T_{\rm PFS}, where each electron or CS fermion splinters off into two quasiparticles, a fermionic chargeon and a bosonic fluxon. The chargeon is nothing but Jain's CF, and the fluxon carries 2q2q units of CS fluxes. At sufficiently low temperatures TTBC(<TPFS)T \leq T_{\rm BC} (< T_{\rm PFS}), fluxons Bose-condense uniformly and (partly) cancel the external magnetic field, producing the correlation holes. This partial cancellation validates the mean-field theory in Jain's CF approach. FQHE takes place at T<TBCT < T_{\rm BC} as a joint effect of (i) integer QHE of chargeons under the residual field ΔB\Delta B and (ii) Bose condensation of fluxons. We calculate the phase-transition temperature TPFST_{\rm PFS} and the CF mass. PFS is a counterpart of the charge-spin separation in the t-J model of high-TcT_{\rm c} cuprates in which each electron dissociates into holon and spinon. Quasiexcitations and resistivity in the PFS state are also studied. The resistivity is just the sum of contributions of chargeons and fluxons, and ρxx\rho_{xx} changes its behavior at T=TPFST = T_{\rm PFS}, reflecting the change of quasiparticles from chargeons and fluxons at T<TPFST < T_{\rm PFS} to electrons at TPFS<TT_{\rm PFS} < T.Comment: 18 pages, 7 figure

    Higher-Energy Composite Fermion Levels in the Fractional Quantum Hall Effect

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    Even though composite fermions in the fractional quantum Hall liquid are well established, it is not yet known up to what energies they remain intact. We probe the high-energy spectrum of the 1/3 liquid directly by resonant inelastic light scattering, and report the observation of a large number of new collective modes. Supported by our theoretical calculations, we associate these with transitions across two or more composite fermions levels. The formation of quasiparticle levels up to high energies is direct evidence for the robustness of topological order in the fractional quantum Hall effect
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