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Phys. Rev. Lett. 100, 227001 (2008) [4 pages]

Phase Diagram of the Electron-Doped La2-xCexCuO4 Cuprate Superconductor from Andreev Bound States at Grain Boundary Junctions

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M. Wagenknecht*, D. Koelle, and R. Kleiner
Physikalisches Institut—Experimentalphysik II and Center for Collective Quantum Phenomena, Universität Tübingen, Auf der Morgenstelle 14, D-72076 Tübingen, Germany

S. Graser and N. Schopohl
Institut für Theoretische Physik, Universität Tübingen, Auf der Morgenstelle 14, D-72076 Tübingen, Germany

B. Chesca
Department of Physics, Loughborough University, Loughborough, Leics LE11 3TU, United Kingdom

A. Tsukada
NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243, Japan

S. T. B. Goennenwein and R. Gross
Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, Walther-Meissner Strasse 8, D-85748 Garching, Germany

Received 17 September 2007; published 2 June 2008

We use quasiparticle tunneling across La2-xCexCuO4 grain boundary junctions to probe the superconducting state and its disappearance with increasing temperature and magnetic field. A zero bias conductance peak due to zero energy surface Andreev bound states is a clear signature of the phase coherence of the superconducting state. Hence, such a peak must disappear at or below the upper critical field Bc2(T). For La2-xCexCuO4 this approach sets a lower bound for Bc2(0)≈25  T which is substantially higher than reported previously. The method of probing the superconducting state via Andreev bound states should also be applicable to other cuprate superconductors.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.100.227001
DOI:
10.1103/PhysRevLett.100.227001
PACS:
74.25.Dw, 74.25.Op, 74.45.+c, 74.50.+r

*wagenknecht@uni-tuebingen.de