516 research outputs found

    GINZBURG-LANDAU THEORY OF VORTICES IN dd-WAVE SUPERCONDUCTORS

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    Ginzburg-Landau theory is used to study the properties of single vortices and of the Abrikosov vortex lattice in a dx2−y2d_{x^2-y^2} superconductor. For a single vortex, the ss-wave order parameter has the expected four-lobe structure in a ring around the core and falls off like 1/r21/r^2 at large distances. The topological structure of the ss-wave order parameter consists of one counter-rotating unit vortex, centered at the core, surrounded by four symmetrically placed positive unit vortices. The Abrikosov lattice is shown to have a triangular structure close to TcT_c and an oblique structure at lower temperatures. Comparison is made to recent neutron scattering data.Comment: 4 pages, REVTeX, 3 figures available upon reques

    NMR relaxation time around a vortex in stripe superconductors

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    Site-dependent NMR relaxation time T1(r)T_1({\bf r}) is calculated in the vortex state using the Bogoliubov-de Gennes theory, taking account of possible "field-induced stripe'' states in which the magnetism arises locally around a vortex core in d-wave superconductivity. The recently observed huge enhancement T1−1(r)T_1^{-1}({\bf r}) below TcT_c at a core site in Tl2_2Ba2_2CuO6_6 is explained. The field-induced stripe picture explains consistently other relevant STM and neutron experiments.Comment: 4 pages, 4 figure

    The Effects of Phase Separation in the Cuprate Superconductors

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    Phase separation has been observed by several different experiments and it is believed to be closely related with the physics of cuprates but its exactly role is not yet well known. We propose that the onset of pseudogap phenomenon or the upper pseudogap temperature T∗T^* has its origin in a spontaneous phase separation transition at the temperature Tps=T∗T_{ps}=T^*. In order to perform quantitative calculations, we use a Cahn-Hilliard (CH) differential equation originally proposed to the studies of alloys and on a spinodal decomposition mechanism. Solving numerically the CH equation it is possible to follow the time evolution of a coarse-grained order parameter which satisfies a Ginzburg-Landau free-energy functional commonly used to model superconductors. In this approach, we follow the process of charge segregation into two main equilibrium hole density branches and the energy gap normally attributed to the upper pseudogap arises as the free-energy potential barrier between these two equilibrium densities below TpsT_{ps}. This simulation provides quantitative results %on the hole doping and temperature %dependence of the degree of the charge inhomogeneity in agreement with %some experiments and the simulations reproduce the observed stripe and granular pattern of segregation. Furthermore, with a Bogoliubov-deGennes (BdG) local superconducting critical temperature calculation for the lower pseudogap or the onset of local superconductivity, it yields novel interpretation of several non-conventional measurements on cuprates.Comment: Published versio

    ss- and dxyd_{xy}-wave components induced around a vortex in dx2−y2d_{x^2-y^2}-wave superconductors

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    Vortex structure of dx2−y2d_{x^2-y^2}-wave superconductors is microscopically analyzed in the framework of the quasi-classical Eilenberger equations. If the pairing interaction contains an ss-wave (dxyd_{xy}-wave) component in addition to a dx2−y2d_{x^2-y^2}-wave component, the ss-wave (dxyd_{xy}-wave) component of the order parameter is necessarily induced around a vortex in dx2−y2d_{x^2-y^2}-wave superconductors. The spatial distribution of the induced ss-wave and dxyd_{xy}-wave components is calculated. The ss-wave component has opposite winding number around vortex near the dx2−y2d_{x^2-y^2}-vortex core and its amplitude has the shape of a four-lobe clover. The amplitude of dxyd_{xy}-component has the shape of an octofoil. These are consistent with results based on the GL theory.Comment: RevTex,9 pages, 6 figures in a uuencoded fil

    The Structure of a Vortex in the t-J Model

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    We study the single-vortex solution of the t-J model within resonating-valence-bond (RVB) mean-field theory. We find two types of vortex cores, insulating and metallic, depending on the parameters of the model. The pairing order parameter near both cores have dx2−y2+iηdxyd_{x^2 -y^2}+i\eta d_{xy} symmetry. For some range of t/Jt/J the calculated tunneling spectrum of the metallic vortex core agrees qualitatively with the STM tunneling data for BSCCO

    Charge Modulation at the Surface of High-T_c Superconductors

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    It is shown here that surfaces of high-temperature superconductors are covered by dipole layers. The charge density modulation is induced by the local suppression of the gap function at the surface. This effect is studied in the framework of the Ginzburg-Landau theory and crucially depends on the appropriate boundary conditions. Those are derived from Gor'kov's equations for a d-wave pairing symmetry. Within this framework the structure of the surface dipole layer is determined. The contribution of this charging to a lens-effect of superconducting films with holes, which has been studied in recent experiments, is discussed.Comment: 10 pages, RevTeX, 5 postscript figure

    Ginzburg Landau theory for d-wave pairing and fourfold symmetric vortex core structure

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    The Ginzburg Landau theory for d_{x^2-y^2}-wave superconductors is constructed, by starting from the Gor'kov equation with including correction terms up to the next order of ln(T_c/T). Some of the non-local correction terms are found to break the cylindrical symmetry and lead to the fourfold symmetric core structure, reflecting the internal degree of freedom in the pair potential. Using this extended Ginzburg Landau theory, we investigate the fourfold symmetric structure of the pair potential, current and magnetic field around an isolated single vortex, and clarify concretely how the vortex core structure deviates from the cylindrical symmetry in the d_{x^2-y^2}-wave superconductors.Comment: 12 pages including 8 eps figs, LaTeX with jpsj.sty & epsfi

    Theory of NMR as a local probe for the electronic structure in the mixed state of the high-TcT_c cuprates

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    We argue that nuclear magnetic resonance experiments are a site-sensitive probe for the electronic spectrum in the mixed state of the high-TcT_c cuprates. Within a spin-fermion model, we show that the Doppler-shifted electronic spectrum arising from the circulating supercurrent changes the low-frequency behavior of the imaginary part of the spin-susceptibility. For a hexagonal vortex lattice, we predict that these changes lead to {\it (a)} a unique dependence of the 63^{63}Cu spin lattice relaxation rate, 1/T11/T_1, on resonance frequency, and {\it (b)} a temperature dependence of T1T_1 which varies with frequency. We propose a nuclear quadrupole experiment to study the effects of a uniform supercurrent on the electronic structure and predict that T1T_1 varies with the direction of the supercurrent.Comment: RevTex, 5 pages, 3 figures embedded in the tex

    Induction of non-d-wave order-parameter components by currents in d-wave superconductors

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    It is shown, within the framework of the Ginzburg-Landau theory for a superconductor with d_{x^2-y^2} symmetry, that the passing of a supercurrent through the sample results, in general, in the induction of order-parameter components of distinct symmetry. The induction of s-wave and d_{xy(x^2-y^2)-wave components are considered in detail. It is shown that in both cases the order parameter remains gapless; however, the structure of the lines of nodes and the lobes of the order parameter are modified in distinct ways, and the magnitudes of these modifications differ in their dependence on the (a-b plane) current direction. The magnitude of the induced s-wave component is estimated using the results of the calculations of Ren et al. [Phys. Rev. Lett. 74, 3680 (1995)], which are based on a microscopic approach.Comment: 15 pages, includes 2 figures. To appear in Phys. Rev.
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