ar X iv : c on d - m at / 9 50 41 17 v 1 2 8 A pr 1 99 5 Quasiparticle current in ballistic NcS ′ S junctions

ar X iv : c on d - m at / 9 60 40 34 v 1 5 A pr 1 99 6 Josephson and Quasiparticle Tunneling between Anisotropically Paired Superconductors

Charge transport in tunnel junctions between singlet anisotropically paired superconductors is investigated theoretically making use of the Eilenberger equations for the quasiclassical Green functions. For specularly reflecting tunnel barrier plane we have found and described analytically characteristic singular points of the I-V curves which are specific for the case of anisotropic pairing. Al...

ar X iv : c on d - m at / 9 81 02 47 v 1 2 0 O ct 1 99 8 Transport properties of quasiparticles with fractional exclusion statistics

We consider the ballistic transport of quasiparticles with exclusion statistics through a 1D wire within the Landauer-Büttiker approach. We demonstrate that quasiparticle transport coefficients (electrical and heat conductance, as well as thermopower) are determined by the same general formulae as for particles with normal statistics. By applying the developed formalism to the ballistic transpo...

ar X iv : c on d - m at / 9 50 70 27 v 1 1 1 Ju l 1 99 5 Fundamental properties of a vortex in a d - wave superconductor

The vortex core structure in a d-wave superconductor is analyzed on the basis of the quasi-classical Eilenberger theory beyond the Ginzburg-Landau framework. The current and magnetic field distributions around an isolated vortex break circular symmetry seen in s-wave pairing and show four-fold symmetry, reflecting the internal degrees of freedom in d-wave pairing, i.e. ˆ k 2 x − ˆ k 2 y in reci...

ar X iv : c on d - m at / 9 40 10 66 v 1 2 8 Ja n 19 94 Ground state energy and quasiparticle gaps

ar X iv : c on d - m at / 9 41 00 14 v 1 6 O ct 1 99 4 Andreev reflection in ferromagnet – superconductor junctions

The transport properties of a ferromagnet–superconductor (FS) junction are studied in a scattering formulation. Andreev reflection at the FS interface is strongly affected by the exchange interaction in the ferromagnet. The conductance GFS of a ballistic point contact between F and S can be both larger or smaller than the value GFN with the superconductor in the normal state, depending on the r...