Article abstract


Nature Physics 1, 117 - 121 (2005)
doi:10.1038/nphys154

Subject Categories: Condensed-matter physics | Quantum physics

Fate of the Josephson effect in thin-film superconductors

Michael Hermele1, Gil Refael2, Matthew P. A. Fisher2 and Paul M. Goldbart3


The d.c. Josephson effect refers to the dissipationless electrical current—the supercurrent—that can be sustained across a weak link connecting two bulk superconductors. This effect probes the nature of the superconducting state, which depends crucially on spatial dimensionality. For bulk (that is, three-dimensional) superconductors, the superconductivity is most robust and the Josephson effect is sustained even at non-zero temperature. However, in wires and thin films, thermal and quantum fluctuations play a crucial role. In superconducting wires, these effects qualitatively modify the electrical transport across a weak link. Despite several experiments involving weak links between thin-film superconductors, little theoretical attention has been paid to the electrical conduction in such systems. Here, we analyse the case of two superconducting thin films connected by a point contact. Remarkably, the Josephson effect is absent at non-zero temperature. The point-contact resistance is non-zero and varies with temperature in a nearly activated fashion, with a universal energy barrier set by the superfluid stiffness characterizing the films. This behaviour reflects the subtle nature of thin-film superconductors and should be observable in future experiments.

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  1. Department of Physics, University of California Santa Barbara, Santa Barbara, California 93106, USA
  2. Kavli Institute for Theoretical Physics, University of California Santa Barbara, Santa Barbara, California 93106, USA
  3. Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA

Correspondence to: Michael Hermele1 Present address: Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA

Correspondence to: Michael Hermele1 e-mail: hermele@mit.edu

Correspondence to: Gil Refael2 Present address: Department of Physics, California Institute of Technology, Pasadena, California 91125, USA

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