Working Group 9 - Magneto-electronics (WG9 Web pages)
Paul Kelly, U Twente, Netherlands
A new area of research in magnetism, called "Spin Electronics" or "Magnetoelectronics" started with the discovery of the "Giant Magnetoresistance" (GMR) effect in 1988. A new electronics is envisioned in which the electron transport is manipulated using not only the charge of the electron as in conventional electronics, but also using the intrinsic electron spin. Thanks in large part to the work of the European theory groups, which collaborate in this Network, the problem posed by the original GMR effect is now quite well understood. However, new effects continue to be found, even in metallic systems. Current-induced magnetization reversal ("spin transfer") was proposed on theoretical grounds but only recently observed. Understanding it requires studying spin transport in non-collinearly aligned magnetic systems. Tunneling magnetoresistance (TMR) is found in transport through magnetic tunnel junctions with amorphous or epitaxial barriers. Such functions could form the basis for a new non-volatile magnetic random access (MRAM) storage technology. Although leading industrial companies have already working MRAM prototypes and are planning market introduction in 2003/2004, the physical understanding of the effect is still in its infancy. Our ambition for the coming years is to understand the TMR effect well enough to be able to make reliable materials-specific predictions.
To form a link between conventional semiconductor-based electronics and transition metal based spin-electronics, it is necessary to find a way to inject a spin-polarized current from a ferromagnet into a semiconductor. Here reliable calculations for the ferromagnet/semiconductor interface would be very important to understand the nature of the interface states, which determine the Schottky barrier and govern the injection process. Collaboration with WG7 on semiconductors and nano-technology will clearly be important and will be undertaken. An ab-initio search for new half-metallic ferromagnetic alloys with 100% spin polarization at E_f and of their interfaces with semiconductors could be very fruitful. Ab-initio calculations could also play an important role in the search for new dilute ferromagnetic semiconductors with Curie temperatures well above room temperature and/or which can be doped n-type. This could enable an all-semiconductor spin electronics (at present the record Curie temperature stands at 110K for GaMnAs). Finally, understanding the spin dependent transmission at the Ferromagnet/Superconductor interface, i.e. the Andreev reflection,in terms of realistic bandstructures is another ambitious aim. All these problems can be addressed using standard density functional calculations for the ground state, and calculations based on the Kubo-Greenwood or Landauer-Buettiker formalism for the spin-dependent transport.
MEMBERS OF THE WORKING GROUP [12 + 8 others interested]
- Prof. dr. P.J. Kelly (
),
Computational Materials Science, Faculty of Applied Physics and MESA+
Research Institute, University of Twente, P.O. Box 217, 7500 AE Enschede,
The Netherlands - Prof. dr. P.H. Dederichs, Institut fuer Festkoerperforschung, Forschungszentrum Juelich GmbH, D-52425 Julich, Germany
- Dr. I. Turek, Institute of Physics of Materials, Academy of Sciences of the Czech Republic, Zizkova 22, CZ-61662 Brno, Czech Republic
- Prof. dr. I. Mertig, Fachgruppe Theoretische Physik, Fachbereich Physik, Martin-Luther-Iniversitaet, Halle-Wittenberg, D-06099 Halle, Germany
- Prof. dr. P. Weinberger, Center for Computational Materials Science, Gumpendorferstraße 1A,Vienna University of Technology, A-1060 Vienna, Austria
- Prof. Dr. H. Ebert, Universitaet Muenchen, Department Chemie, Physikalische Chemie, Haus E, Butenandtstr. 5-13, D-81377 Muenchen, Germany
- Prof. Dr. P. Bruno, Max-Planck-Institut für Mikrostrukturphysik, Weinberg 2, D-06120 Halle, Germany
- V. Drchal, Institute of Physics, Academy of Sciences of the Czech Republic, CZ-182 21 Prague, Czech Republic
- J. Kudronovsky, Institute of Physics, Academy of Sciences of the Czech Republic, CZ-182 21 Prague, Czech Republic
- L. Szunyogh, Department of Theoretical Physics, Budapest University of Technology and Economics, Budafoki ut. 8, 1521 Budapest, Hungary
- C. J. Lambert, Department of Physics, Lancaster University, Lancaster LA1 4YB, United Kingdom
- N. Stefanou, Section of Solid State Physics, University of Athens, Panepistimioupolis, GR-157 84, Athens, Greece
OTHERS INTERESTED
- W. M. Temmerman, Daresbury Laboratory, Daresbury, Warrington, WA4 4AD, United Kingdom
- J. F. Annett, H. H. Wills Physics Laboratory, University of Bristol, Royal Fort, Tyndall Avenue, Bristol BS8 1TL, United Kingdom
- D. G. Pettifor, Department of Materials, University of Oxford, Oxford OX1 3PH, United Kingdom
- Ch. Sommers, Laboratoire de Physique des Solides, Université de Paris-Sud, 91405 Orsay Cedex, France
- D. Stoeffler, Institut de Physique et Chimie des Matériaux de Strasbourg, UMR CNRS-ULP 7504, 23, rue du Loess, F-67037 Strasbourg, France
- S. Redinger, Center for Computational Materials Science, Technische Universität Wien, Getreidemarkt 9/158, 1060 Vienna, Austria
- G. E. W. Bauer, Department of Applied Physics and DIMES, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, The Netherlands
- Dr. Stefaan Cottenier, Instituut voor Kern- en Stralingsfysica, K.U.Leuven, Celestijnenlaan 200 D, B-3001 Leuven, Belgium