SUPERCONDUCTING ORDER-PARAMETER SYMMETRY IN MULTILAYER CUPRATES

Citation
J. Maly et al., SUPERCONDUCTING ORDER-PARAMETER SYMMETRY IN MULTILAYER CUPRATES, Physical review. B, Condensed matter, 53(10), 1996, pp. 6786-6805
Citations number
67
Categorie Soggetti
Physics, Condensed Matter
ISSN journal
01631829
Volume
53
Issue
10
Year of publication
1996
Pages
6786 - 6805
Database
ISI
SICI code
0163-1829(1996)53:10<6786:SOSIMC>2.0.ZU;2-K
Abstract
We classify the allowed order parameter symmetries in multilayer cupra tes and discuss their physical consequences, with emphasis on Josephso n tunneling and impurity scattering. Our solutions to the gap equation are based on highly nonspecific forms for the inter- and intraplane p airing interactions in order to arrive at the most general conclusions . Within this framework, the bilayer (N = 2) case is discussed in deta il with reference to Y-Ba-Cu-O (YBCO) and Bi-Sr-Ca-Cu-O (BSCCO) and th e related Landau-Ginzburg free energy functional. Particular attention is paid to the role of small orthorhombic distortions as would derive from the chains in YBCO and from superlattice effects in BSCCO, which give rise to a rich and complex behavior of the multilayer order para meter. This order parameter has N components associated with each of t he N bands or layers. Moreover, these components have specific phase r elationships. In the orthorhombic bilayer case the (s, - s) State is o f special interest, since for a wide range of phase space, this state exhibits rr phase shifts in corner Josephson junction experiments. In addition, its transition temperature is found to be insensitive to non magnetic interplane disorder, as would be present at the rare earth si te in YBCO, for example. Of particular interest, also, are the role of van Hove singularities which are seen to stabilize states with d(x)2( -y)2-like Symmetry (as well as nodeless s states) and to elongate the gap functions along the four van Hove points, thereby leading to a sub stantial region of gaplessness. We find that for these rather general models of the pairing interaction the d(x)2(-y)2-like states are the m ost stable solutions in a large region of parameter space. In this way , they should not be specifically associated with a spin fluctuation d riven pairing mechanism.