110 research outputs found

    Comment on "T-dependence of the magnetic penetration depth in unconventional superconductors at low temperatures: Can it be linear?"

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    We show that the clean superconductor with line of gap nodes is not in conflict with the Nernst theorem. The answer to the question in the title of the Schopohl-Dolgov paper in Phys. Rev. Lett. 80 (1998) 4761 (cond-mat/9802264) is yes.Comment: Comment to the paper by Schopohl and Dolgov in Phys. Rev. Lett. 80 (1998) 4761 (cond-mat/9802264), RevTex file, 1 page, no figures, typos are corrected, submitted to Phys. Rev. Let

    Comment on "Is the nonlinear Meissner effect unobservable?"

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    In a recent Letter (Phys. Rev. Lett. 81, p.5640 (1998), cond-mat/9808249 v3), it was suggested that nonlocal effects may prevent observation of the nonlinear Meissner effect in YBCO. We argue that this claim is incorrect with regards to measurements of the nonlinear transverse magnetic moment, and that the most likely reason for a null result lies elsewhere.Comment: 1 pag

    Multiple stochastic pathways in forced peptide-lipid membrane detachment

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    We have used high resolution AFM based dynamic force spectroscopy to investigate peptide-lipid membrane interactions by measuring the detachment (last-rupture) force distribution, P(F), and the corresponding force dependent rupture rate, k(F), for two different peptides and lipid bilayers. The measured quantities, which differed considerably for different peptides, lipid-membranes, AFM tips (prepared under identical conditions), and retraction speeds of the AFM cantilever, could not be described in terms of the standard theory, according to which detachment occurs along a single pathway, corresponding to a diffusive escape process across a free energy barrier. In particular, the prominent retraction speed dependence of k(F) was a clear indication that peptide-lipid membrane dissociation occurs stochastically along several detachment pathways. Thereby, we have formulated a general theoretical approach for describing P(F) and k(F), by assuming that peptide detachment from lipid membranes occurs, with certain probability, along a few dominant diffusive pathways. This new method was validated through a consistent interpretation of the experimental data. Furthermore, we have found that for moderate retraction speeds at intermediate force values, k(F) exhibits catch-bond behavior (i.e. decreasing detachment rate with increasing force). According to the proposed model this behavior is due to the stochastic mixing of individual detachment pathways which do not convert or cross during rupture. To our knowledge, such catch-bond mechanism has not been proposed and demonstrated before for a peptide-lipid interaction

    Non-Locality and Strong Coupling in the Heavy Fermion Superconductor CeCoIn5_{5}: A Penetration Depth Study

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    We report measurements of the magnetic penetration depth λ\lambda in single crystals of CeCoIn5_{5} down to \sim0.14 K using a tunnel-diode based, self-inductive technique at 28 MHz. While the in-plane penetration depth tends to follow a power law, λ//T3/2\lambda_{//} \sim {\it T}^{3/2}, the data are better described as a crossover between linear ({\it T} \gg T{\it T}^\ast ) and quadratic ({\it T} T\ll {\it T}^\ast ) behavior, with T{\it T}^\ast the crossover temperature in the strong-coupling limit. The {\it c}-axis penetration depth λ\lambda_{\perp} is linear in {\it T}, providing evidence that CeCoIn5_{5} is a {\it d}-wave superconductor with line nodes along the {\it c}-axis. The different temperature dependences of λ//\lambda_{//} and λ\lambda_{\perp} rule out impurity effects as the source of T{\it T}^{\ast} .Comment: 4 pages, 3 figure

    Pairing Fluctuation Theory of Superconducting Properties in Underdoped to Overdoped Cuprates

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    We propose a theoretical description of the superconducting state of under- to overdoped cuprates, based on the short coherence length of these materials and the associated strong pairing fluctuations. The calculated TcT_c and the zero temperature excitation gap Δ(0)\Delta(0), as a function of hole concentration xx, are in semi-quantitative agreement with experiment. Although the ratio Tc/Δ(0)T_c/\Delta(0) has a strong xx dependence, different from the universal BCS value, and Δ(T)\Delta(T) deviates significantly from the BCS prediction, we obtain, quite remarkably, quasi-universal behavior, for the normalized superfluid density ρs(T)/ρs(0)\rho_s(T)/\rho_s(0) and the Josephson critical current Ic(T)/Ic(0)I_c(T)/I_c(0), as a function of T/TcT/T_c. While experiments on ρs(T)\rho_s(T) are consistent with these results, future measurements on Ic(T)I_c(T) are needed to test this prediction.Comment: 4 pages, 3 figures, REVTeX, submitted to Phys. Rev. Let

    Phase Fluctuations and Pseudogap Properties: Influence of Nonmagnetic Impurities

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    The presence of nonmagnetic impurities in a 2D ``bad metal'' depresses the superconducting Berezinskii-Kosterlitz-Thouless transition temperature, while leaving the pairing energy scale unchanged. Thus the region of the pseudogap non-superconducting phase, where the modulus of the order parameter is non-zero but its phase is random, and which opens at the pairing temperature is substantially bigger than for the clean system. This supports the premise that fluctuations in the phase of the order parameter can in principle describe the pseudogap phenomena in high-TcT_c materials over a rather wide range of temperatures and carrier densities. The temperature dependence of the bare superfluid density is also discussed.Comment: 11 pages, LaTeX, 1 EPS figure; final version to appear in Low.Temp.Phy

    On the T-dependence of the magnetic penetration depth in unconventional superconductors at low temperatures: can it be linear?

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    We present a thermodynamics argument against a strictly linear temperature dependence of the magnetic penetration depth, which applies to superconductors with arbitrary pairing symmetry at low temperatures.Comment: 5 pages, expanded version of cond-mat/971102

    Superconductivity in the quasi-two-dimensional Hubbard model

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    On the basis of spin and pairing fluctuation-exchange approximation, we study the superconductivity in quasi-two-dimensional Hubbard model. The integral equations for the Green's function are self-consistently solved by numerical calculation. Solutions for the order parameter, London penetration depth, density of states, and transition temperature are obtained. Some of the results are compared with the experiments for the cuprate high-temperature superconductors. Numerical techniques are presented in details. With these techniques, the amount of numerical computation can be greatly reduced.Comment: 17 pages, 13 figure

    Interlayer Coupling and p-wave Pairing in Strontium Ruthenate

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    On the basis of a three orbital model and an effective attractive interaction between electrons we investigate the possible superconducting states, with pp and ff-wave internal symmetry, of Sr2_2RuO4_4. For an orbital dependent interaction which acts between in plane and out of plane nearest neighbour Ruthenium atoms we find a state for which the gap in the quasi-particle spectra has a line node on the α\alpha and β\beta sheets of the Fermi Surface, but it is complex with no nodes on the γ\gamma-sheet. We show that this state is consistent with all the available experimental data. In particular, we present the results of our calculations of the specific heat and penetration depth as functions of the temperature.Comment: 4 pages, 5 figure

    Evidence for Surface Andreev Bound states in Cuprate Superconductors from Penetration Depth Measurements

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    Tunneling and theoretical studies have suggested that Andreev bound states form at certain surfaces of unconventional superconductors. Through studies of the temperature and field dependence of the in-plane magnetic penetration depth lambda_ab at low temperature, we have found strong evidence for the presence of these states in clean single crystal YBCO and BSCCO. Crystals cut to expose a [110] interface show a strong upturn in lambda_ab at around 7K, when the field is oriented so that the supercurrents flow around this surface. In YBCO this upturn is completely suppressed by a field of ~0.1 T.Comment: 4 pages 2 column revtex + 4 postscript figures. Submitted to PR
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