288 research outputs found

    Spin-charge-lattice coupling near the metal-insulator transition in Ca3Ru2O7

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    We report x-ray scattering studies of the c-axis lattice parameter in Ca3Ru2O7 as a function of temperature and magnetic field. These structural studies complement published transport and magnetization data, and therefore elucidate the spin-charge-lattice coupling near the metal-insulator transition. Strong anisotropy of the structural change for field applied along orthogonal in-plane directions is observed. Competition between a spin-polarized phase that does not couple to the lattice, and an antiferromagnetic metallic phase, which does, gives rise to rich behavior for B ∥\parallel b.Comment: 6 pages, 4 figures, to appear in Phys. Rev.

    Absence of orbital-selective Mott transition in Ca_2-xSr_xRuO4

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    Quasi-particle spectra of the layer perovskite Sr2_2RuO4_4 are calculated within Dynamical Mean Field Theory for increasing values of the on-site Coulomb energy UU. At small UU the planar geometry splits the t2gt_{2g} bands near EFE_F into a wide, two-dimensional dxyd_{xy} band and two narrow, nearly one-dimensional dxz,yzd_{xz,yz} bands. At larger UU, however, the spectral distribution of these states exhibit similar correlation features, suggesting a common metal-insulator transition for all t2gt_{2g} bands at the same critical UU.Comment: 4 pages, 4 figure

    Rigid-Band Shift of the Fermi Level in a Strongly Correlated Metal: Sr(2-y)La(y)RuO(4)

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    We report a systematic study of electron doping of Sr2RuO4 by non-isovalent substitution of La^(3+) for Sr^(2+). Using a combination of de Haas-van Alphen oscillations, specific heat, and resistivity measurements, we show that electron doping leads to a rigid-band shift of the Fermi level corresponding to one doped electron per La ion, with constant many-body quasiparticle mass enhancement over the band mass. The susceptibility spectrum is substantially altered and enhanced by the doping but this has surprisingly little effect on the strength of the unconventional superconducting pairing.Comment: 4 pages, 3 figure

    Spectroscopy of SrRuO/Ru Junctions in Eutectic

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    We have investigated the tunnelling properties of the interface between superconducting Sr2RuO4 and a single Ru inclusion in eutectic. By using a micro-fabrication technique, we have made Sr2RuO4/Ru junctions on the eutectic system that consists of Sr2RuO4 and Ru micro-inclusions. Such a eutectic system exhibits surface superconductivity, called the 3-K phase. A zero bias conductance peak (ZBCP) was observed in the 3-K phase. We propose to use the onset of the ZBCP to delineate the phase boundary of a time-reversal symmetry breaking state.Comment: To be published in Proc of 24th Int. Conf. on Low Temperature Physics (LT24); 2 page

    Orbital-dependent metamagnetic response in Sr4Ru3O10

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    We show that the metamagnetic transition in Sr4_4Ru3_3O10_{10} bifurcates into two transitions as the field is rotated away from the conducting planes. This two-step process comprises partial or total alignment of moments in ferromagnetic bands followed by an itinerant metamagnetic transition whose critical field increases with rotation. Evidence for itinerant metamagnetism is provided by the Shubnikov-de Hass effect which shows a non-trivial evolution of the geometry of the Fermi surface and an enhancement of the quasiparticles effective-mass across the transition. The metamagnetic response of Sr4_4Ru3_3O10_{10} is orbital-dependent and involves ferromagnetic and metamagnetic bands.Comment: Physical Review B (in press

    Anisotropy of the incommensurate fluctuations in Sr2RuO4: a study with polarized neutrons

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    The anisotropy of the magnetic incommensurate fluctuations in Sr2RuO4 has been studied by inelastic neutron scattering with polarized neutrons. We find a sizeable enhancement of the out of plane component by a factor of two for intermediate energy transfer which appears to decrease for higher energies. Our results qualitatively confirm calculations of the spin-orbit coupling, but the experimental anisotropy and its energy dependence are weaker than predicted.Comment: 4 pages, 4 figure
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