Letter

Nature 441, 486-488 (25 May 2006) | doi:10.1038/nature04778; Received 13 September 2005; Accepted 29 March 2006

Detection of magnetic circular dichroism using a transmission electron microscope

P. Schattschneider1, S. Rubino1, C. Hébert1, J. Rusz2, J. Kunes caron2, P. Novák2, E. Carlino3, M. Fabrizioli3,4, G. Panaccione3 and G. Rossi3,5

A material is said to exhibit dichroism if its photon absorption spectrum depends on the polarization of the incident radiation. In the case of X-ray magnetic circular dichroism (XMCD), the absorption cross-section of a ferromagnet or a paramagnet in a magnetic field changes when the helicity of a circularly polarized photon is reversed relative to the magnetization direction. Although similarities between X-ray absorption and electron energy-loss spectroscopy in a transmission electron microscope (TEM) have long been recognized, it has been assumed that extending such equivalence to circular dichroism would require the electron beam in the TEM to be spin-polarized. Recently, it was argued on theoretical grounds that this assumption is probably wrong1. Here we report the direct experimental detection of magnetic circular dichroism in a TEM. We compare our measurements of electron energy-loss magnetic chiral dichroism (EMCD) with XMCD spectra obtained from the same specimen that, together with theoretical calculations, show that chiral atomic transitions in a specimen are accessible with inelastic electron scattering under particular scattering conditions. This finding could have important consequences for the study of magnetism on the nanometre and subnanometre scales, as EMCD offers the potential for such spatial resolution down to the nanometre scale while providing depth information—in contrast to X-ray methods, which are mainly surface-sensitive.

  1. Service Centre for Transmission Electron Microscopy, Wiedner Hauptstrae 8-10/052, and Institut für Festkörperphysik, Wiedner Hauptstrae 8-10/138, Technische Universität Wien, A-1040 Wien, Austria
  2. Institute of Physics ASCR, Cukrovarnická 10, 16253 Praha 6, Czech Republic
  3. TASC INFM-CNR National Laboratory, Area Science Park, S.S.14, Km 163.5, I-34012 Trieste, Italy
  4. Università degli Studi di Trieste, Piazzale Europa 1, I-34100 Trieste, Italy
  5. Dipartimento di Fisica dell'Università di Modena e Reggio Emilia–I-41100 Modena, Italy

Correspondence to: P. Schattschneider1 Correspondence and requests for materials should be addressed to P.S. (Email: schatt@ifp.tuwien.ac.at).

Received 13 September 2005 | Accepted 29 March 2006

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