Synopsis: Dirac connection

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Illustration: J. K. Asbóth et al., Phys. Rev. B (2009)

Pseudodiffusive transmission of nodal Dirac fermions through a clean d-wave superconductor

J. K. Asbóth, A. R. Akhmerov, A. C. Berceanu, and C. W. J. Beenakker

Published December 18, 2009

In response to a voltage, the electrical current in a pure sheet of graphene diminishes as 1/L, where L is the length over which the current is transmitted. This form of scaling, called pseudodiffusive because of its similarity to diffusion in a random potential, occurs when L is less than the width of the sheet and the mean free path.

In graphene, pseudodiffusion occurs because the electrons behave like massless Dirac fermions. Now, in a paper appearing in Physical Review B, János Asbóth and collaborators at Leiden University in the Netherlands calculate the transmission of electrons and holes between two normal-metal electrodes, separated over a distance L by a clean d-wave superconductor. Asbóth et al. find that the transmitted electrical and thermal currents both have the pseudodiffusive 1/L scaling characteristic of massless Dirac fermions—regardless of the presence of tunnel barriers at the metal-superconductor interfaces—as long as L is larger than the superconducting coherence length and smaller than the width of the superconductor and the mean free path. This occurs because the d-wave superconductor forms ballistic conduction channels for coupled electron-hole excitations that are described by an anisotropic two-dimensional Dirac equation analogous to that of graphene. This finding is likely to spur experimental efforts to search for pseudodiffusive transmission in clean single crystals of high-Tc cuprates. – Sarma Kancharla

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