Titlebook: Electron Correlation in New Materials and Nanosystems; Kurt Scharnberg,Sergei Kruchinin Conference proceedings 20071st edition Springer Sc

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Raymond B. Seymour,Gerald S. Kirshenbauming of .- and .-wave symmetry of the superconducting order parameter in order to describe orthorhombic superconductors. We compare our calculations with new experimental data on fully untwinned YBa.Cu.O. and find good agreement. Our results are in contrast to earlier interpretations on the in-plane anisotropy in terms of stripes.

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II.1 Magnesium diboride and the two-band scenarioa path integral approach. A definition of the critical level spacing of the two-gap superconductivity is also presented, and we discuss condensation energy and parity gap of the two-gap superconductivity in relation to the size dependence of those properties with two bulk gaps and effective pair scattering process between two sublevels.

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G. Geiser,H. Foysi,W. Schr?der,M. Meinkeed with the change of the Fermi surface dimensionality of one of the superlattice subbands. The case of light element diborides where Mg is substituted for Al in AlB. and its similarity with intercalated graphite compounds is discussed.

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SQL Server In-Memory Technologiesspin response in the coexisting DDW and d..-..-wave superconducting (DSC) states and discuss the peculiar features of the resonance peak dispersion. Furthermore, we investigate the infuence of various tight-binding parameters and the orthorhombic distortions on the robustness of the features discussed.

CIS

Toshiki Iwasaki,Masahiro Sawadathe non-ballistic (not spectral) regime of current flow in the nanocontacts. Thus, the current induced magnetoconductance effects in multilayered N–F structures (nanopillars) extensively studied in the recent literature have much more general character and can be stimulated by elastic electron scattering at single N–F interfaces.

MUT

MAGNETIC UNIPOLAR FEATURES IN CONDUCTIVITY OF POINT CONTACTS BETWEEN NORMAL AND FERROMAGNETIC D-METAthe non-ballistic (not spectral) regime of current flow in the nanocontacts. Thus, the current induced magnetoconductance effects in multilayered N–F structures (nanopillars) extensively studied in the recent literature have much more general character and can be stimulated by elastic electron scattering at single N–F interfaces.