24 research outputs found

    Search for Cooper-pair Fluctuations in Severely Underdoped YBCO Films

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    The preformed-pairs theory of pseudogap physics in high-TCT_C superconductors predicts a nonanalytic TT-dependence for the abab-plane superfluid fraction, ρS\rho_S, at low temperatures in underdoped cuprates. We report high-precision measurements of ρS(T)\rho_S(T) on severely underdoped YBa2_2Cu3_3O6+x_{6+x} and Y0.8_{0.8}Ca0.2_{0.2}Ba2_2Cu3_3O6+x_{6+x} films. At low TT, ρS\rho_S looks more like 1T21 - T^2 than 1T3/21 - T^{3/2}, in disagreement with theory.Comment: 3 pages, 2 figure

    Superfluid density of superconductor-ferromagnet bilayers

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    We report the first measurements of the effective superfluid density n_S(T) \propto \lambda^{-2}(T) of Superconductor-Ferromagnet (SC/FM) bilayers, where \lambda is the effective magnetic field penetration depth. Thin Nb/Ni bilayers were sputtered in ultrahigh vacuum in quick succession onto oxidized Si substrates. Nb layers are 102 A thick for all samples, while Ni thicknesses vary from 0 to 100 A. T_C determined from \lambda^{-2}(T) decreases rapidly as Ni thickness d_Ni increases from zero to 15 A, then it has a shallow minimum at d_Ni \approx 25 A. \lambda^{-2}(0) behaves similarly, but has a minimum several times deeper. In fact, \lambda^{-2}(0) continues to increase with increasing Ni thickness long after T_C has stopped changing. We argue that this indicates a substantial superfluid density inside the ferromagnetic Ni films.Comment: 13 pages, 2 figures, MMM 2007 proceeding

    Anomalously Sharp Superconducting Transitions in Overdoped La2xSrxCuO4La_{2-x}Sr_{x}CuO_{4} Films

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    We present measurements of abab-plane resistivity ρab(T)\rho_{ab}(T) and superfluid density [λ2\propto \lambda^{-2}, λ\lambda = magnetic penetration depth] in La2xSrxCuO4La_{2-x}Sr_{x}CuO_{4} films. As Sr concentration xx exceeds about 0.22, the superconducting transition sharpens dramatically, becoming as narrow as 200 mK near the super-to-normal metal quantum critical point. At the same time, ρab(T)\rho_{ab}(T), λ2(T)\lambda^{-2}(T), and transition temperature TcT_c decrease, and upward curvature develops in λ2(T)\lambda^{-2}(T). Given the sharp transitions, we interpret these results in the context of a homogeneous d-wave superconducting state, with elastic scattering that is enhanced relative to underdoped LSCO due to weaker electron correlations. This interpretation conflicts with the viewpoint that the overdoped state is inhomogeneous due to phase separation into superconducting and normal metal regions.Comment: 21 pages including 3 figures and 56 references. This version includes responses to referees and slight correction of data on two films. Conclusions the same as befor

    Field-dependent diamagnetic transition in magnetic superconductor Sm1.85Ce0.15CuO4ySm_{1.85} Ce_{0.15} Cu O_{4-y}

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    The magnetic penetration depth of single crystal Sm1.85Ce0.15CuO4y\rm{Sm_{1.85}Ce_{0.15}CuO_{4-y}} was measured down to 0.4 K in dc fields up to 7 kOe. For insulating Sm2CuO4\rm{Sm_2CuO_4}, Sm3+^{3+} spins order at the N\'{e}el temperature, TN=6T_N = 6 K, independent of the applied field. Superconducting Sm1.85Ce0.15CuO4y\rm{Sm_{1.85}Ce_{0.15}CuO_{4-y}} (Tc23T_c \approx 23 K) shows a sharp increase in diamagnetic screening below T(H)T^{\ast}(H) which varied from 4.0 K (H=0H = 0) to 0.5 K (H=H = 7 kOe) for a field along the c-axis. If the field was aligned parallel to the conducting planes, TT^{\ast} remained unchanged. The unusual field dependence of TT^{\ast} indicates a spin freezing transition that dramatically increases the superfluid density.Comment: 4 pages, RevTex

    Fourfold oscillations and anomalous magnetic irreversibility of magnetoresistance in the non-metallic regime of Pr1.85Ce0.15CuO4

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    Using magnetoresistance measurements as a function of applied magnetic field and its direction of application, we present sharp angular-dependent magnetoresistance oscillations for the electron-doped cuprates in their low-temperature non-metallic regime. The presence of irreversibility in the magnetoresistance measurements and the related strong anisotropy of the field dependence for different in-plane magnetic field orientations indicate that magnetic domains play an important role for the determination of electronic properties. These domains are likely related to the stripe phase reported previously in hole-doped cuprates.Comment: 11 pages, 5 figure

    Quantum oscillations from Fermi arcs

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    When a metal is subjected to strong magnetic field B nearly all measurable quantities exhibit oscillations periodic in 1/B. Such quantum oscillations represent a canonical probe of the defining aspect of a metal, its Fermi surface (FS). In this study we establish a new mechanism for quantum oscillations which requires only finite segments of a FS to exist. Oscillations periodic in 1/B occur if the FS segments are terminated by a pairing gap. Our results reconcile the recent breakthrough experiments showing quantum oscillations in a cuprate superconductor YBCO, with a well-established result of many angle resolved photoemission (ARPES) studies which consistently indicate "Fermi arcs" -- truncated segments of a Fermi surface -- in the normal state of the cuprates.Comment: 8 pages, 5 figure

    Single and two-particle energy gaps across the disorder-driven superconductor-insulator transition

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    The competition between superconductivity and localization raises profound questions in condensed matter physics. In spite of decades of research, the mechanism of the superconductor-insulator transition (SIT) and the nature of the insulator are not understood. We use quantum Monte Carlo simulations that treat, on an equal footing, inhomogeneous amplitude variations and phase fluctuations, a major advance over previous theories. We gain new microscopic insights and make testable predictions for local spectroscopic probes. The energy gap in the density of states survives across the transition, but coherence peaks exist only in the superconductor. A characteristic pseudogap persists above the critical disorder and critical temperature, in contrast to conventional theories. Surprisingly, the insulator has a two-particle gap scale that vanishes at the SIT, despite a robust single-particle gap.Comment: 7 pages, 5 figures (plus supplement with 4 pages, 5 figures
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