430 research outputs found

    Spectroscopy and critical temperature of diffusive superconducting/ferromagnetic hybrid structures with spin-active interfaces

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    The description of the proximity effect in superconducting/ferromagnetic heterostructures requires to use spin-dependent boundary conditions. Such boundary conditions must take into account the spin dependence of the phase shifts acquired by electrons upon scattering on the boundaries of ferromagnets. The present article shows that this property can strongly affect the critical temperature and the energy dependence of the density of states of diffusive heterostructures. These effects should allow a better caracterisation of diffusive superconductor/ferromagnet interfaces.Comment: 12 pages, 6 figures, to be published in Phys. Rev.

    Effect of disorder on the far-infrared conductivity and on the microwave conductivity of two-band superconductors

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    We consider the far-infrared and the microwave conductivities of a two-band superconductor with non-magnetic impurities. The strong coupling expressions for the frequency and temperature dependent conductivity of a two-band superconductor are developed assuming isotropic bands and interactions. Our numerical results obtained using realistic interaction parameters for MgB2_{2} are compared with experiments on this compound. We find that the available experimental results for the far-infrared conductivity of MgB2_{2} are consistent with multi-band superconductivity in the presence of a sufficiently strong interband impurity scattering. On the other hand, our numerical results for the microwave conductivity in the superconducting state indicate that the experimental results obtained on samples with the highest transition temperature TcT_{c} are consistent with a low interband impurity scattering rate but depend sensitively on the ratio of the total scattering rates in the two bands. For the π\pi-band scattering rate γπ\gamma_{\pi} not greater than the σ\sigma-band scattering rate γσ\gamma_{\sigma} there is a single, broad, low-temperature (at about 0.5TcT_{c}) coherence peak in the microwave conductivity. For γπ/γσ\gamma_{\pi}/\gamma_{\sigma}=4--7 a high-temperature (at about 0.9TcT_{c}) coherence peak is dominant, but there is also a low-temperature peak/shoulder resulting from the contribution of the π\pi-band carriers to the microwave conductivity. For γπ/γσ≫\gamma_{\pi}/\gamma_{\sigma}\gg1 only the high-temperature coherence peak should be observable.Comment: 11 pages, 6 figure

    Proximity effect in the presence of Coulomb interaction and magnetic field

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    We consider a small metallic grain coupled to a superconductor by a tunnel contact. We study the interplay between proximity and charging effects in the presence of the external magnetic field. Employing the adiabatic approximation we develop a self-consistent theory valid for an arbitrary ratio of proximity and Coulomb strength. The magnetic field suppresses the proximity-induced minigap in an unusual way. We find the phase diagram of the grain in the charging energy - magnetic field plane. Two distinct states exist with different values and magnetic field dependences of the minigap. The first-order phase transition occurs between these two minigapped states. The transition to the gapless state may occur by the first- or second-order mechanism depending on the charging energy. We also calculate the tunneling density of states in the grain. The energy dependence of this quantity demonstrates two different gaps corresponding to the Coulomb and proximity effects. These gaps may be separated in sufficiently high magnetic field.Comment: 11 pages (including 8 EPS figures). Version 3: extended. Final version as published in PR

    Theory of tunneling spectroscopy of normal metal/ferromagnet/spin-triplet superconductor junctions

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    We study the tunneling conductance of a ballistic normal metal / ferromagnet / spin-triplet superconductor junction using the extended Blonder-Tinkham-Klapwijk formalism as a model for a cc-axis oriented Au / SrRuO3_{3} / Sr2_{2}RuO4_{4} junction. We compare chiral pp-wave (CPW) and helical pp-wave (HPW) pair potentials, combined with ferromagnet magnetization directions parallel and perpendicular to the interface. For fixed θM\theta_{M}, where θM\theta_{M} is a direction of magnetization in the ferromagnet measured from the cc-axis, the tunneling conductance of CPW and HPW clearly show different voltage dependencies. It is found that the cases where the dd-vector is perpendicular to the magnetization direction (CPW with θM=π/2\theta_{M} = \pi/2 and HPW with θM=0\theta_{M} = 0) are identical. The obtained results serve as a guide to determine the pairing symmetry of the spin-triplet superconductor Sr2_{2}RuO4_{4}.Comment: 12 pages, 7 figures. There is also a supplementary (not uploaded

    Competitive 0 and {\pi} states in S/F multilayers: multimode approach

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    We have investigated the critical temperature behavior in periodic superconductor/ ferromagnet (S/F) multilayers as a function of the ferromagnetic layer thickness dfd_f and the interface transparency. The critical temperature Tc(df)T_c(d_f) exhibits a damped oscillatory behavior in these systems due to an exchange field in the ferromagnetic material. In this work we have performed TcT_c calculations using the self-consistent multimode approach, which is considered to be exact solving method. Using this approach we have derived the conditions of 0 or π\pi state realization in periodic S/F multilayers. Moreover, we have presented the comparison between the single-mode and multimode approaches and established the limits of applicability of the single-mode approximation, frequently used by experimentalists

    Eliashberg approach to superconductivity-induced infrared anomalies in Ba0.68K0.32Fe2As2

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    We report the full complex dielectric function of high-purity Ba0.68K0.32Fe2As2\textrm{Ba}_{0.68}\textrm{K}_{0.32}\textrm{Fe}_2\textrm{As}_2 single crystals with Tc=38.5 KT_{\mathrm{c}}=38.5\ \textrm{K} determined by wide-band spectroscopic ellipsometry at temperatures 10≤T≤300 K10\leq T\leq300\ \textrm{K}. We discuss the microscopic origin of superconductivity-induced infrared optical anomalies in the framework of a multiband Eliashberg theory with two distinct superconducting gap energies $2\Delta_{\mathrm{A}}\approx6\ k_{\mathrm{B}}T_{\mathrm{c}}and and 2\Delta_{\mathrm{B}}\approx2.2\ k_{\mathrm{B}}T_{\mathrm{c}}.Theobservedunusualsuppressionoftheopticalconductivityinthesuperconductingstateatenergiesupto. The observed unusual suppression of the optical conductivity in the superconducting state at energies up to 14\ k_{\mathrm{B}}T_{\mathrm{c}}$ can be ascribed to spin-fluctuation--assisted processes in the clean limit of the strong-coupling regime.Comment: 4 pages, 4 figures; suppl. material: 3 pages, 2 figures, 1 interactive simulation (Fig. S3

    Radiation linewidth of a long Josephson junction in the flux-flow regime

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    Theoretical model for the radiation linewidth in a multi-fluxon state of a long Josephson junction is presented. Starting from the perturbed sine-Gordon model with the temperature dependent noise term, we develop a collective coordinate approach which allows to calculate the finite radiation linewidth due to excitation of the internal degrees of freedom in the moving fluxon chain. At low fluxon density, the radiation linewidth is expected to be substantially larger than that of a lumped Josephson oscillator. With increasing the fluxon density, a crossover to a much smaller linewidth corresponding to the lumped oscillator limit is predicted.Comment: 11 pages LaTeX, to appear in Phys Rev
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