987 research outputs found

    Fate of the Bose insulator in the limit of strong localization and low Cooper-pair density in ultrathin films

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    A Bose insulator composed of a low density of strongly localized Cooper pairs develops at the two-dimensional superconductor to insulator transition (SIT) in a number of thin film systems. Investigations of ultrathin amorphous PbBi films far from the SIT described here provide evidence that the Bose insulator gives way to a second insulating phase with decreasing film thickness. At a critical film thickness dc the magnetoresistance changes sign from positive, as expected for boson transport, to negative, as expected for fermion transport, signs of local Cooper-pair phase coherence effects on transport vanish, and the transport activation energy exhibits a kink. Below dc pairing fluctuation effects remain visible in the high-temperature transport while the activation energy continues to rise. These features show that Cooper pairing persists and suggest that the localized unpaired electron states involved in transport are interspersed among regions of strongly localized Cooper pairs in this strongly localized, low Cooper-pair density phase

    Collapse of the Cooper pair phase coherence length at a superconductor to insulator transition

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    We present investigations of the superconductor to insulator transition (SIT) of uniform a-Bi films using a technique sensitive to Cooper pair phase coherence. The films are perforated with a nanohoneycomb array of holes to form a multiply connected geometry and subjected to a perpendicular magnetic field. Film magnetoresistances on the superconducting side of the SIT oscillate with a period dictated by the superconducting flux quantum and the areal hole density. The oscillations disappear close to the SIT critical point to leave a monotonically rising magnetoresistance that persists in the insulating phase. These observations indicate that the Cooper pair phase coherence length, which is infinite in the superconducting phase, collapses to a value less than the interhole spacing at this SIT. This behavior is inconsistent with the gradual reduction of the phase coherence length expected for a bosonic, phase fluctuation driven SIT. This result starkly contrasts with previous observations of oscillations persisting in the insulating phase of other films implying that there must be at least two distinct classes of disorder tuned SITs

    Magnetic Flux Periodic Response of Nano-perforated Ultrathin Superconducting Films

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    We have patterned a hexagonal array of nano-scale holes into a series of ultrathin, superconducting Bi/Sb films with transition temperatures 2.65 K <Tco<<T_{co} < 5 K. These regular perforations give the films a phase-sensitive periodic response to an applied magnetic field. By measuring this response in their resistive transitions, R(T)R(T), we are able to distinguish regimes in which fluctuations of the amplitude, both the amplitude and phase, and the phase of the superconducting order parameter dominate the transport. The portion of R(T)R(T) dominated by amplitude fluctuations is larger in lower TcoT_{co} films and thus, grows with proximity to the superconductor to insulator transition.Comment: Revised title, abstract, text, figure

    Effect of Magnetic Impurities on Suppression of the Transition Temperature in Disordered Superconductors

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    We calculate the first-order perturbative correction to the transition temperature TcT_c in a superconductor with both non-magnetic and magnetic impurities. We do this by first evaluating the correction to the effective potential, Ω(Δ)\Omega(\Delta), and then obtain the first-order correction to the order parameter, Δ\Delta, by finding the minimum of Ω(Δ)\Omega(\Delta). Setting Δ=0\Delta=0 finally allows TcT_c to be evaluated. TcT_c is now a function of both the resistance per square, R□R_\square, a measure of the non-magnetic disorder, and the spin-flip scattering rate, 1/τs1/\tau_s, a measure of the magnetic disorder. We find that the effective pair-breaking rate per magnetic impurity is virtually independent of the resistance per square of the film, in agreement with an experiment of Chervenak and Valles. This conclusion is supported by both the perturbative calculation, and by a non-perturbative re-summation technique.Comment: 29 pages, 9 figure

    Josephson junction array type I-V characteristics of quench-condensed ultra thin films of Bi

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    In this communication we report studies of d.c current-voltage (I-V) characteristics of ultra thin films of Bi, quench condensed on single crystal sapphire substrates at T = 15K. The hysteretic I-V characteristics are explained using a resistively and capacitively shunted junction (RCSJ) model of Josephson junction arrays. The Josephson coupling energy(EJE_J) and the charging energy(EcE_c) are calculated for different thickness(dd) values. A low resistance state is found in the low current regime below the critical current, IcI_c. This resistance R0R_0 is found to have a minimum at a particular thickness (dcd_c) value. Reflection High Energy Electron Diffraction (RHEED) studies are done on these films. A distinct appearance of a diffuse ring near dcd_c is observed in the diffraction images, consistent with the recent STM studies(Ekinci and Valles, PRL {\bf 82}(1999) 1518). These films show an irreversible annealing when temperature is increased. The annealing temperature (TaT_a) also has a maximum at the same thickness. Althoguh the Rs_s vs T of quench condensed Bi films suggest that the films are uniform, our results indicate that even in thick films, the order parameter is not fully developed over the complete area of the film. These results are discussed qualitatively.Comment: 6 pages, 6 figure

    Weak anisotropic impurity scattering in unconventional superconductors

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    The effect of weak anisotropic (momentum-dependent) impurity scattering in unconventional superconductors has been investigated. It is shown that the anisotropic scattering can lead either to a small reduction or a small enhancement of the isotropic pair-breaking effect. The influence of the anisotropy of the scattering potential becomes significant for the order parameters with large Fermi surface average values. In that case an unexpected enhancement (up to 10%) of the critical temperature over the critical temperature in the absence of impurities is predicted for a small impurity concentration.Comment: 12 pages, RevTeX, 3 PostScript figure
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