12,365 research outputs found

    Momentum-resolved charge excitations in high-Tc cuprates studied by resonant inelastic x-ray scattering

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    We report a Cu K-edge resonant inelastic x-ray scattering (RIXS) study of high-Tc cuprates. Momentum-resolved charge excitations in the CuO2 plane are examined from parent Mott insulators to carrier-doped superconductors. The Mott gap excitation in undoped insulators is found to commonly show a larger dispersion along the [pi,pi] direction than the [pi,0] direction. On the other hand, the resonance condition displays material dependence. Upon hole doping, the dispersion of the Mott gap excitation becomes weaker and an intraband excitation appears as a continuum intensity below the gap at the same time. In the case of electron doping, the Mott gap excitation is prominent at the zone center and a dispersive intraband excitation is observed at finite momentum transfer

    Observation of Conduction Band Satellite of Ni Metal by 3p-3d Resonant Inverse Photoemission Study

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    Resonant inverse photoemission spectra of Ni metal have been obtained across the Ni 3pp absorption edge. The intensity of Ni 3dd band just above Fermi edge shows asymmetric Fano-like resonance. Satellite structures are found at about 2.5 and 4.2 eV above Fermi edge, which show resonant enhancement at the absorption edge. The satellite structures are due to a many-body configuration interaction and confirms the existence of 3d8d^8 configuration in the ground state of Ni metal.Comment: 4 pages, 3 figures, submitted to Physical Review Letter

    Static quark free energies at finite temperature with two flavors of improved Wilson quarks

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    Polyakov loop correlations at finite temperature in two-flavor QCD are studied in lattice simulations with the RG-improved gluon action and the clover-improved Wilson quark action. From the simulations on a 163×416^3 \times 4 lattice, we extract the free energies, the effective running coupling geff(T)g_{\rm eff}(T) and the Debye screening mass mD(T)m_D(T) for various color channels of heavy quark--quark and quark--anti-quark pairs above the critical temperature. The free energies are well approximated by the screened Coulomb form with the appropriate Casimir factors. The magnitude and the temperature dependence of the Debye mass are compared to those of the next-to-leading order thermal perturbation theory and to a phenomenological formula given in terms of geff(T)g_{\rm eff}(T). Also we made a comparison between our results with the Wilson quark and those with the staggered quark previously reported.Comment: 7 pages, 9 figures, talk given at Lattice 2006 (high temperature and density

    Finite temperature phase transition of two-flavor QCD with an improved Wilson quark action

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    We study the phase structure of QCD at finite temperatures with two flavors of dynamical quarks on a lattice with the size Ns3×Nt=163×4N_s^3 \times N_t=16^3 \times 4, using a renormalization group improved gauge action and a clover improved Wilson quark action. The simulations are made along the lines of constant physics determined in terms of mPS/mVm_{\rm PS}/m_{\rm V} at zero-temperature. We show preliminary results for the spatial string tension in the high temperature phase.Comment: 7 pages, 7 figures, talk presented at Lattice 2006 (high temperature and density

    Thermodynamics and heavy-quark free energies at finite temperature and density with two flavors of improved Wilson quarks

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    Thermodynamics of two-flavor QCD at finite temperature and density is studied on a 163×416^3 \times 4 lattice, using a renormalization group improved gauge action and the clover improved Wilson quark action. In the simulations along lines of constant mPS/mVm_{\rm PS}/m_{\rm V}, we calculate the Taylor expansion coefficients of the heavy-quark free energy with respect to the quark chemical potential (ÎŒq\mu_q) up to the second order. By comparing the expansion coefficients of the free energies between quark(QQ)and antiquark(Qˉ\bar{Q}), and between QQ and QQ, we find a characteristic difference at finite ÎŒq\mu_q due to the first order coefficient of the Taylor expansion. We also calculate the quark number and isospin susceptibilities, and find that the second order coefficient of the quark number susceptibility shows enhancement around the pseudo-critical temperature.Comment: Talk given at the XXV International Symposium on Lattice Field Theory (Lattice 2007), July 30 - August 4, 2007, Regensburg, German

    Mott gap excitations in twin-free YBa2Cu3O7-d (Tc = 93 K) studied by RIXS

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    Mott gap excitations in the high-Tc superconductor of the optimal doped YBa2Cu3O7-d (Tc = 93 K) have been studied by the resonant inelastic x-ray scattering method. Anisotropic spectra in the ab-plane are observed in a twin-free crystal. The excitation from the one-dimensional CuO chain is enhanced at 2 eV near the zone boundary of the b* direction, while the excitation from the CuO2 plane is broad at 1.5-4 eV and almost independent of the momentum transfer. Theoretical calculation based on the one-dimensional and two-dimensional Hubbard model reproduces the observed spectra by taking the different parameters of the on-site Coulomb energy. The fact of the Mott gap of the CuO chain site is much smaller than that of CuO2 plane site is observed for the first time

    Nuclear Force from Monte Carlo Simulations of Lattice Quantum Chromodynamics

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    The nuclear force acting between protons and neutrons is studied in the Monte Carlo simulations of the fundamental theory of the strong interaction, the quantum chromodynamics defined on the hypercubic space-time lattice. After a brief summary of the empirical nucleon-nucleon (NN) potentials which can fit the NN scattering experiments in high precision, we outline the basic formulation to derive the potential between the extended objects such as the nucleons composed of quarks. The equal-time Bethe-Salpeter amplitude is a key ingredient for defining the NN potential on the lattice. We show the results of the numerical simulations on a 32432^4 lattice with the lattice spacing a≃0.137a \simeq 0.137 fm (lattice volume (4.4 fm)4^4) in the quenched approximation. The calculation was carried out using the massively parallel computer Blue Gene/L at KEK. We found that the calculated NN potential at low energy has basic features expected from the empirical NN potentials; attraction at long and medium distances and the repulsive core at short distance. Various future directions along this line of research are also summarized.Comment: 13 pages, 4 figures, version accepted for publication in "Computational Science & Discovery" (IOP
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