28,396 research outputs found

    Broken-Symmetry States of Dirac Fermions in Graphene with A Partially Filled High Landau Level

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    We report on numerical study of the Dirac fermions in partially filled N=3 Landau level (LL) in graphene. At half-filling, the equal-time density-density correlation function displays sharp peaks at nonzero wavevectors ±q\pm {\bf q^{*}}. Finite-size scaling shows that the peak value grows with electron number and diverges in the thermodynamic limit, which suggests an instability toward a charge density wave. A symmetry broken stripe phase is formed at large system size limit, which is robust against purturbation from disorder scattering. Such a quantum phase is experimentally observable through transport measurements. Associated with the special wavefunctions of the Dirac LL, both stripe and bubble phases become possible candidates for the ground state of the Dirac fermions in graphene with lower filling factors in the N=3 LL.Comment: Contains are slightly changed. Journal reference and DOI are adde

    Odd-Integer Quantum Hall Effect in Graphene: Interaction and Disorder Effects

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    We study the competition between the long-range Coulomb interaction, disorder scattering, and lattice effects in the integer quantum Hall effect (IQHE) in graphene. By direct transport calculations, both ν=1\nu=1 and ν=3\nu=3 IQHE states are revealed in the lowest two Dirac Landau levels. However, the critical disorder strength above which the ν=3\nu=3 IQHE is destroyed is much smaller than that for the ν=1\nu=1 IQHE, which may explain the absence of a ν=3\nu=3 plateau in recent experiments. While the excitation spectrum in the IQHE phase is gapless within numerical finite-size analysis, we do find and determine a mobility gap, which characterizes the energy scale of the stability of the IQHE. Furthermore, we demonstrate that the ν=1\nu=1 IQHE state is a Dirac valley and sublattice polarized Ising pseudospin ferromagnet, while the ν=3\nu=3 state is an xyxy plane polarized pseudospin ferromagnet.Comment: 5 pages, 5 figure

    Classical integrability of the O(N) nonlinear Sigma model on a half-line

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    The classical integrability the O(N) nonlinear sigma model on a half-line is examined, and the existence of an infinity of conserved charges in involution is established for the free boundary condition. For the case N=3 other possible boundary conditions are considered briefly.Comment: 12 Pages. Latex file (process twice

    Quantum Spin Hall Effect and Topologically Invariant Chern Numbers

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    We present a topological description of quantum spin Hall effect (QSHE) in a two-dimensional electron system on honeycomb lattice with both intrinsic and Rashba spin-orbit couplings. We show that the topology of the band insulator can be characterized by a 2×22\times 2 traceless matrix of first Chern integers. The nontrivial QSHE phase is identified by the nonzero diagonal matrix elements of the Chern number matrix (CNM). A spin Chern number is derived from the CNM, which is conserved in the presence of finite disorder scattering and spin nonconserving Rashba coupling. By using the Laughlin's gedanken experiment, we numerically calculate the spin polarization and spin transfer rate of the conducting edge states, and determine a phase diagram for the QSHE.Comment: 4 pages and 4 figure

    Spatially Resolved Nonlinearity Measurements of YBa2_2Cu3_3O7d_{7-d} Bi-crystal Grain Boundaries

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    We have developed a near-field microwave microscope to locally excite a superconducting film and measure second and third harmonic responses at microwave frequencies. We study the local nonlinear response of a YBa2_2Cu3_3O7d_{7-d} thin film grown on a bi-crystal SrTiO3_3 substrate. The location of the bi-crystal grain boundary is clearly identified by the microscope through higher harmonic response, and the spatial resolution is on the order of the magnetic loop probe size, about 500μm\mu m. The harmonic power and spatial resolution are successfully modeled with a one-dimensional extended Josephson junction simulation. From the model, the 2nd order harmonic response is dominated by Josephson vortex generation and flow. A geometry-free nonlinear scaling current density JNL104105A/cm2J_{NL}\simeq 10^4\sim 10^5 A/cm^2 is also exstracted from the data, indicating that the grain boundary weak link is the dominant nonlinear source in this case.Comment: 4pages, 4figure
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