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Energy-loss magnetic chiral dichroism (EMCD): Magnetic chiral dichroism in the electron microscope
Uppsala University, Disciplinary Domain of Science and Technology, Technology, Department of Engineering Sciences, Experimental Physics.
Institute for Solid State Physics, Vienna University of Technology, Vienna A-1040, Austria; and Service Centre for TEM, Vienna University of Technology, Vienna A-1040, Austria.
Service Centre for TEM, Vienna University of Technology, Vienna A-1040, Austria.
SB-CIME Station 12, EPFL, Lausanne, Switzerland.
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2008 (English)In: Journal of Materials Research, ISSN 0884-2914, E-ISSN 2044-5326, Vol. 23, no 10, 2582-2590 p.Article, review/survey (Refereed) Published
Abstract [en]

A new technique called energy-loss magnetic chiral dichroism (EMCD) has recently been developed [P. Schattschneider, et al. Nature 441, 486 (2006)] to measure magnetic circular dichroism in the transmission electron microscope (TEM) with a spatial resolution of 10 nm. This novel technique is the TEM counterpart of x-ray magnetic circular dichroism, which is widely used for the characterization of magnetic materials with synchrotron radiation. In this paper we describe several experimental methods that can be used to measure the EMCD signal [P. Schattschneider, et al. Nature 441, 486 (2006); C. Hébert, et al. Ultramicroscopy 108(3), 277 (2008); B. Warot-Fonrose, et al. Ultramicroscopy 108(5), 393 (2008); L. Calmels, et al. Phys. Rev. B 76, 060409 (2007); P. van Aken, et al. Microsc. Microanal. 13(3), 426 (2007)] and give a review of the recent improvements of this new investigation tool. The dependence of the EMCD on several experimental conditions (such as thickness, relative orientation of beam and sample, collection and convergence angle) is investigated in the transition metals iron, cobalt, and nickel. Different scattering geometries are illustrated; their advantages and disadvantages are detailed, together with current limitations. The next realistic perspectives of this technique consist of measuring atomic specific magnetic moments, using suitable spin and orbital sum rules, [L. Calmels, et al. Phys. Rev. B 76, 060409 (2007); J. Rusz, et al. Phys. Rev. B 76, 060408 (2007)] with a resolution down to 2 to 3 nm.

Place, publisher, year, edition, pages
2008. Vol. 23, no 10, 2582-2590 p.
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Physical Sciences Engineering and Technology
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URN: urn:nbn:se:uu:diva-113951DOI: 10.1557/JMR.2008.0348ISI: 000259785300002OAI: oai:DiVA.org:uu-113951DiVA: diva2:292322
Available from: 2010-02-05 Created: 2010-02-05 Last updated: 2017-12-12Bibliographically approved

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