skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Intralayer-versus-interlayer pairing in the copper oxide superconductors

Journal Article · · Physical Review, B: Condensed Matter; (United States)
 [1];  [2]
  1. Materials Science Division, Argonne National Laboratory, Argonne, Illinois (USA) Solid State Division, Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennessee (USA)
  2. Solid State Division, Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennessee (USA)

We have investigated the competing roles of intralayer {ital s}-wave and interlayer BCS-like pairing in determining the {ital c}-axis versus {ital ab}-plane energy-gap anisotropy in layered superconductors with {ital N}=1,2 conducting planes per unit-cell edge {ital s}. For {ital N}=1, intralayer {ital s}-wave pairing leads to a conventional order parameter (OP) {Delta}{sub 0} with a transition temperature ({ital T}{sub {ital c}}) value {ital T}{sub {ital c}0} and isotropic energy gap 2{vert bar}{Delta}{sub 0}{vert bar}. For interlayer pairing, the four-vector gap function {tilde {Delta}}{sub 3}({ital k}{sub {ital z}}) contains a singlet OP {Delta}{sub {ital s}} and a vector triplet OP {Delta}{sub {ital t}}, with corresponding normalized gap functions {radical}2 cos{ital k}{sub {ital z}s} and {radical}2 sin{ital k}{sub {ital z}s}. Since {Delta}{sub {ital s}} and {Delta}{sub {ital t}} have identical {ital T}{sub {ital c}} values ({ital T}{sub {ital c}{ital s}}={ital T}{sub {ital c}{ital t}}), the free energy is minimized when {vert bar}{Delta}{sub {ital s}}{vert bar}={vert bar}{Delta}{sub {ital t}}{vert bar}, and the resulting gap 2{vert bar}{Delta}{vert bar} is found to be {ital isotropic}. However, 2{vert bar}{Delta}{vert bar} is completely {ital incompatible} with 2{vert bar}{Delta}{sub 0}{vert bar}. For {ital N}=2, there are two intralayer pairing OP's {Delta}{sub 0} and {Delta}{sub 1}, and two interlayer four-vector gap functions {tilde {Delta}}{sub 3}({ital k}{sub {ital z}}) and {tilde {Delta}}{sub 2}({ital k}{sub {ital z}}), all of which could contribute to measurable quantities in the Gaussian-fluctuation regime above the highest {ital T}{sub {ital c}} value.

Research Organization:
Argonne National Laboratory (ANL), Argonne, IL
DOE Contract Number:
AC05-84OR21400; W-31109-ENG-38; W-7405-ENG-82
OSTI ID:
5127044
Journal Information:
Physical Review, B: Condensed Matter; (United States), Vol. 44:14; ISSN 0163-1829
Country of Publication:
United States
Language:
English