Mise en page 1 - Laboratoire National des Champs Magnétiques ...

TABLE OF CONTENTSPreface 1Carbon Allotropes 3Investigation of the dynamic alignment of single walled carbon nanotubes in pulsed high magnetic fields . . 5Charge transport mechanisms in arrays of multi-walled carbon nanotubes . . . . . . . . . . . . . . . . . . 6Propagative Landau states and Fermi level pinning in carbon nanotubes . . . . . . . . . . . . . . . . . . . 7Aharonov-Bohm modulation of the high energy subbands in carbon nanotubes . . . . . . . . . . . . . . . . 8Edge fingerprints and magneto-conductance in graphene nanoribbons . . . . . . . . . . . . . . . . . . . . 9Using Landau quantization to suppress Auger scattering in graphene . . . . . . . . . . . . . . . . . . . . . 10Observation of the half-integer quantum Hall effect in epitaxial graphene . . . . . . . . . . . . . . . . . . . 11Integer quantum Hall effect in epitaxial graphene . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12Improving graphene’s cleanliness for high field magneto-transport . . . . . . . . . . . . . . . . . . . . . . 13Metal-insulator transition for filling factor ν = −2 to ν = 0 in graphene . . . . . . . . . . . . . . . . . . . 14How perfect can graphene be? . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15Effect of a magnetic field on the two-phonon Raman scattering in graphene . . . . . . . . . . . . . . . . . 16Tuning the electron-phonon coupling in graphene with magnetic fields . . . . . . . . . . . . . . . . . . . . 17Thermal conductivity of graphene in Corbino membrane geometry . . . . . . . . . . . . . . . . . . . . . . 18Electric field doping of few-layer graphene . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19Low temperature magneto-transport in natural graphite . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20Magnetotransport to extract the spin gap for charged excitations in graphite . . . . . . . . . . . . . . . . . 21Magneto-transmission spectroscopy of graphite in high magnetic fields . . . . . . . . . . . . . . . . . . . . 22Graphite from the viewpoint of Landau level spectroscopy: An effective graphene bilayer and monolayer . . 23Magneto-transmission of multi-layer epitaxial graphene and bulk graphite: A comparison . . . . . . . . . . 24Two-Dimensional Electron Gas 25The surprisingly fragile quantum Hall ferromagnet at filling factor ν = 1 . . . . . . . . . . . . . . . . . . . 27Dispersive line shape of the resistively detected NMR on either side of filling factor ν = 1 . . . . . . . . . . 28Spin splitting enhancement of fully populated Landau levels . . . . . . . . . . . . . . . . . . . . . . . . . 29Spin polarisation of a disordered GaAs 2D electron gas in a strong in-plane magnetic field . . . . . . . . . 30High-order fractional microwave induced resistance oscillations . . . . . . . . . . . . . . . . . . . . . . . 31Crossover between distinct mechanisms of microwave photoconductivity in double quantum wells . . . . . 32Emergent fractional quantum Hall effect in a triple quantum well . . . . . . . . . . . . . . . . . . . . . . . 33Reentrant fractional quantum Hall states in a triple quantum well . . . . . . . . . . . . . . . . . . . . . . . 34Magneto-intersubband oscillations in multilayer electron systems . . . . . . . . . . . . . . . . . . . . . . . 35