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Sergei Sergeenkov

Publications and source records attributed to Sergei Sergeenkov.

24 records · Page 2Linked to original sources

Novel Effects in High-Tc Granular Superconductors Predicted via Model of 3D Josephson Junction Arrays

Despite the fact that Josephson Junction Arrays (JAA) have been actively studied for decades, they continue to contribute to the variety of intriguing and peculiar phenomena (both fundamental and important for potential applications) providing at the same time a useful tool for testing new theoretical ideas. To give just a few recent examples, it is sufficient to mention paramagnetic Meissner effect (PME) as well as the recently introduced thermophase and piezophase effects suggesting, respectively, a direct influence of a thermal gradient and an applied stress on phase difference between the adjacent grains. At the same time, an artificially prepared islands of superconducting grains, well-described by the various models of JJAs, proved useful in studying the charging effects in these systems, ranging from Coulomb blockade of Cooper pair tunneling and Bloch oscillations to propagation of quantum ballistic vortices. The present paper reviews some of the recently suggested novel effects which should manifest themselves either in weak-links-bearing superconductors or in artificially prepared JJAs. In Section 2 we consider the appearance of an electric-field induced magnetization (analog of the so-called magnetoelectric effect) in a model granular superconductor. The dual effect, that is an appearance of a magnetic field induced electric polarization is studied in Section 3. Finally, in Section 4 we discuss a possibility of two other interesting effects which are expected to occur in a granular material under mechanical loading. Specifically, we predict the existence of stress induced paramagnetic moment in zero applied magnetic field (Josephson piezomagnetism) and study its influence on a low-field magnetization (leading to a mechanically induced PME).

cond-mat.supr-con↗

Phase dependent differential thermopower of SND junctions: Pair-breaking effects and Gaussian fluctuations

We start with revisiting our previous results on thermoelectric response of SNS configuration in a C-shaped Bi(x)Pb(1-x)Sr(2)CaCu(2)O(y) sample in order to include strong fluctuation effects. Then, by appropriate generalization of the Ginzburg-Landau theory based on admixture of s-wave and d-wave superconductors, we consider a differential thermoelectric power (TEP) of SND junction. In addition to its strong dependence on the relative phase θ=ϕ_s-ϕ_d between the two superconductors, two major effects are shown to influence the behavior of the predicted TEP. One, based on the chemical imbalance at SD interface, results in a pronounced maximum of the TEP peak near θ=π/2 (where the so-called s+id mixed pairing state is formed) for two identical superconductors (with T_d=T_s\equiv T_c). Another effect, which should manifest itself at SD interface comprising an s-wave low-T_c superconductor and a d-wave high-T_c superconductor (with T_d\neq T_s), predicts S_p\propto T_d-T_s for the TEP peak value. The experimental conditions under which the predicted behavior of the induced differential TEP can be measured are discussed.

cond-mat.supr-con↗

Probing mixed s+id pairing state via thermoelectric response of SND junction

The thermoelectric response of SND configuration is considered within the generalized Ginzburg-Landau theory for a homogeneous admixture of s-wave and d-wave superconductors. The resulting thermopower (TP) is found to strongly depend on the relative phase θ=ϕ_s-ϕ_d between the two superconductors. Two independent mechanisms are shown to contribute to the TP. One, based on the charge imbalance between the quasiparticles and Cooper pairs (described by the corresponding chemical potentials) due to the normal metal insert, results in a pronounced maximum of the peak near θ=π/2 (the so-called s+id mixed pairing state) for two identical superconductors with T_{cd}=T_{cs}. This mechanism can be realized in a d-wave orthorhombic sample (like YBCO) with twin boundaries represented by tetragonal regions of variable width, with a reduced chemical potential. Another mechanism (not related to the charge imbalance effects) occurs when two different superconductors with T_{cd}>T_{cs} are used for SND junction. It can be realized via the junction comprising an s-wave low-T_c superconductor (like Pb) and a d-wave high-T_c superconductor (like orthorhombic YBCO). The experimental conditions under which the predicted behavior of the induced differential thermopower can be measured are discussed.

cond-mat.supr-con↗

Nonlinear Seebeck Effect in a Model Granular Superconductor

The change of the Josephson supercurrent density of a weakly-connected granular superconductor in response to externally applied arbitrary thermal gradient dT/dx (nonlinear Seebeck effect) is considered within a model of 3D Josephson junction arrays. For dT/dx>(dT/dx)_c, where (dT/dx)_c is estimated to be of the order of 10^4 K/m for YBCO ceramics with an average grain's size of 10 microns, the weak-links-dominated thermopower S (Seebeck coefficient) is predicted to become strongly dT/dx-dependent.

cond-mat.supr-con↗

On piezophase effects in mechanically loaded atomic scale Josephson junctions

The response of an intrinsic Josephson contact to externally applied stress is considered within the framework of the dislocation-induced atomic scale Josephson effect. The predicted quasi-periodic (Fraunhofer-like)stress-strain and stress-current patterns should manifest themselves for experimentally accessible values of applied stresses in intrinsically defected (e.g.,twinned) crystals.

cond-mat.supr-con↗

On Electrostriction of a Granular Superconductor

Zero-temperature field-induced polarization, supercurrent density, and the related electrostriction (ES) of a granular superconductor are calculated within a model of 3D Josephson junction arrays. Both the "bulk-modulus-driven ES" (the change of the sample's volume in the free energy upon the applied stress) and the "change-of-phase ES" (due to the stress dependence of the weak-links-induced polarization) are considered. In contrast to magnetostriction of a granular superconductor, its electroelastic behavior is predicted to be dominated by the former contribution for all applied fields.

cond-mat.supr-con↗