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Magnetic interference patterns in 0-pi superconductor/insulator/ferromagnet/superconductor Josephson junctions: Effects of asymmetry between 0 and pi regions

Source: Phys. Rev. B 81, 054522 (2010); doi:10.1103/PhysRevB.81.054522

Published 26 February 2010

PACS
  • 74.50.+r
    Superconductor tunneling phenomena; point contacts, weak links, Josephson effects
  • 74.78.Fk
    Superconducting multilayers, superlattices, heterostructures
  • 85.25.Cp
    Josephson devices
  • YEAR: 2010
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
M. Kemmler,1 M. Weides,2 M. Weiler,3 M. Opel,3 S. T. B. Goennenwein,3 A. S. Vasenko,4 A. A. Golubov,5 H. Kohlstedt,6 D. Koelle,1 R. Kleiner,1 and E. Goldobin1
1Physikalisches Institut–Experimentalphysik II and Center for Collective Quantum Phenomena, Universität Tübingen, Auf der Morgenstelle 14, D-72076 Tübingen, Germany
2Institute of Solid State Research and JARA–Fundamentals of Future Information Technology, Research Centre Jülich, D-52425 Jülich, Germany
3Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, D-85748 Garching, Germany
4LPMMC, Université Joseph Fourier and CNRS, 25 Avenue des Martyrs, BP 166, 38042 Grenoble, France
5Faculty of Science and Technology and MESA+ Institute for Nanotechnology, University of Twente, 7500 AE Enschede, The Netherlands
6Nanoelektronik, Technische Fakultät, Christian-Albrechts-Universität zu Kiel, D-24143 Kiel, Germany

We present a detailed analysis of the dependence of the critical current Ic on an in-plane magnetic field B of 0, pi, and 0-pi superconductor-insulator-ferromagnet-superconductor Josephson junctions. Ic(B) of the 0 and the pi junction closely follows a Fraunhofer pattern, indicating a homogeneous critical current density jc(x). The maximum of Ic(B) is slightly shifted along the field axis, pointing to a small remanent in-plane magnetization of the F-layer along the field axis. Ic(B) of the 0-pi junction exhibits the characteristic central minimum. Ic, however, has a finite value here, due to an asymmetry of jc in the 0 and the pi part. In addition, this Ic(B) exhibits asymmetric maxima and bumped minima. To explain these features in detail, flux penetration being different in the 0 part and the pi part needs to be taken into account. We discuss this asymmetry in relation to the magnetic properties of the F-layer and the fabrication technique used to produce the 0-pi junctions. ©2010 The American Physical Society
History: Received 27 October 2009; revised 4 February 2010; published 26 February 2010
Permalink: http://link.aps.org/abstract/PRB/v81/e054522
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