9,693 research outputs found

    Study of gossamer superconductivity and antiferromagnetism in the t-J-U model

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    The d-wave superconductivity (dSC) and antiferromagnetism are analytically studied in a renormalized mean field theory for a two dimensional t-J model plus an on-site repulsive Hubbard interaction UU. The purpose of introducing the UU term is to partially impose the no double occupancy constraint by employing the Gutzwiller approximation. The phase diagrams as functions of doping ÎŽ\delta and UU are studied. Using the standard value of t/J=3.0t/J=3.0 and in the large UU limit, we show that the antiferromagnetic (AF) order emerges and coexists with the dSC in the underdoped region below the doping Ύ∌0.1\delta\sim0.1. The dSC order parameter increases from zero as the doping increases and reaches a maximum near the optimal doping Ύ∌0.15\delta\sim0.15. In the small UU limit, only the dSC order survives while the AF order disappears. As UU increased to a critical value, the AF order shows up and coexists with the dSC in the underdoped regime. At half filing, the system is in the dSC state for small UU and becomes an AF insulator for large UU. Within the present mean field approach, We show that the ground state energy of the coexistent state is always lower than that of the pure dSC state.Comment: 7 pages, 8 figure

    Fermi surface evolution in the antiferromagnetic state for the electron-doped t-t'-t''-J model

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    By use of the slave-boson mean-field approach, we have studied the electron-doped t-t'-t''-J model in the antiferromagnetic (AF) state. It is found that at low doping the Fermi surface (FS) pockets appear around (±π,0)(\pm\pi,0) and (0,±π)(0,\pm\pi), and upon increasing doping the other ones will form around (±π2,±π2)(\pm{\pi\over 2},\pm{\pi\over 2}). The evolution of the FS with doping as well as the calculated spectral weight are consistent with the experimental results.Comment: Fig. 4 is updated, to appear in Phys. Rev.

    Fluctuations in the transmission properties of a quantum dot with interface roughness and impurities

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    We examine statistical fluctuations in the transmission properties of quantum dots with interface roughness and neutral impurities. For this purpose we employ a supercell model of quantum transport capable of simulating potential variations in three dimensions. We find that sample to sample variations in interface roughness in a quantum dot waveguide can lead to substantial fluctuations in the n=1 transmission resonance position, width and maximum. We also find that a strongly attractive impurity near the centre of a quantum dot can reduce these fluctuations. Nevertheless, the presence of more than a single impurity can give rise to a complex resonance structure that varies with impurity configuration

    The temperature dependence of the local tunnelling conductance in cuprate superconductors with competing AF order

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    Based on the t−tâ€Č−U−Vt-t'-U-V model with proper chosen parameters for describing the cuprate superconductors, it is found that near the optimal doping at low temperature (TT), only the pure d-wave superconductivity (ddSC) prevails and the antiferromagnetic (AF) order is completely suppressed. At higher TT, the AF order with stripe modulation and the accompanying charge order may emerge, and they could exist above the ddSC transition temperature. We calculate the local differential tunnelling conductance (LDTC) from the local density of states (LDOS) and show that their energy variations are rather different from each other as TT increases. Although the calculated modulation periodicity in the LDTC/LDOS and bias energy dependence of the Fourier amplitude of LDTC in the "pseudogap" region are in good agreement with the recent STM experiment [Vershinin etal.et al., Science {\bf 303}, 1995 (2004)], we point out that some of the energy dependent features in the LDTC do not represent the intrinsic characteristics of the sample

    Spin dynamics in the antiferromagnetic phase for electron-doped cuprate superconductors

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    Based on the tt-tâ€Čt'-tâ€Čâ€Čt''-JJ model we have calculated the dynamical spin susceptibilities in the antiferromagnetic (AF) phase for electron-doped cuprates, by use of the slave-boson mean-field theory and random phase approximation. Various results for the susceptibilities versus energy and momentum have been shown at different dopings. At low energy, except the collective spin-wave mode around (π,π)(\pi,\pi) and 0, we have primarily observed that new resonance peaks will appear around (0.3π,0.7π)(0.3\pi,0.7\pi) and equivalent points with increasing doping, which are due to the particle-hole excitations between the two AF bands. The peaks are pronounced in the transverse susceptibility but not in the longitudinal one. These features are predicted for neutron scattering measurements.Comment: 5 pages, 3 figures, published version with minor change

    The unique rapid variabilities of the iron Kα\alpha line profiles in NGC 4151

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    We present a detailed analysis of the iron Kα\alpha line variabilities in NGC 4151 by using long ASCA observation data obtained in May 1995. Despite the relatively small amplitude variations in the continuum flux, the iron Kα\alpha line flux and profile show dramatic variations. Particularly, the line profile changes from single peak to seeming double peaks and back in time scales of a few 104^4 sec. The seemingly double-peaked profiles can be well interpreted as line emission from a Keplerian ring around a massive black hole. An absorption line at around 5.9 keV is also marginnaly detected. We discussed current Fe K line models, but none of them can well explain the observed line and continuum variations.Comment: 18 pages, latex, 3 figures, ApJ accepte

    Conductance Characteristics between a Normal Metal and a Superconductor Carrying a Supercurrent

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    The low-temperature conductance (G) characteristics between a normal metal and a clean superconductor (S) carrying a supercurrent IsI_s parallel to the interface is theoretically investigated. Increasing IsI_s causes lowering and broadening of (1) coherence peaks of s-wave S, and d-wave S at (100) contact, (2) midgap-states-induced zero-bias conductance peak for d-wave S at (110) contact, and (3) Andreev-reflection-induced enhancement of GG within the gap near the metallic-contact limit. Novel features found include a current-induced central peak and a three-humped structure at intermediate barrier strength, etc.Comment: 4 pages, 4 figure
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