A High-Pressure Structure in Curium Linked to Magnetism

Author:

Heathman S.12345,Haire R. G.12345,Le Bihan T.12345,Lindbaum A.12345,Idiri M.12345,Normile P.12345,Li S.12345,Ahuja R.12345,Johansson B.12345,Lander G. H.12345

Affiliation:

1. European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125, Karlsruhe, Germany.

2. Oak Ridge National Laboratory (ORNL), Chemical Sciences Division, Office Box 2008, MS-6375, Oak Ridge, TN 37831, USA.

3. European Synchrotron Radiation Facility (ESRF), Boîte Postale 220, F-38043 Grenoble, France.

4. Vienna University of Technology, Institute for Solid State Physics, Wiedner Hauptstrasse 8-10/138, A-1040, Vienna, Austria.

5. Department of Physics, Uppsala University, Box 530, S-751 21 Uppsala, Sweden.

Abstract

Curium lies at the center of the actinide series and has a half-filled shell with seven 5 f electrons spatially residing inside its radon core. As a function of pressure, curium exhibits five different crystallographic phases up to 100 gigapascals, of which all but one are also found in the preceding element, americium. We describe here a structure in curium, Cm III, with monoclinic symmetry, space group C2/c , found at intermediate pressures (between 37 and 56 gigapascals). Ab initio electronic structure calculations agree with the observed sequence of structures and establish that it is the spin polarization of curium's 5 f electrons that stabilizes Cm III. The results reveal that curium is one of a few elements that has a lattice structure stabilized by magnetism.

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

Reference22 articles.

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2. M. S. S. Brooks, B. Johansson, H. L. Skriver, in Handbook on the Physics and Chemistry of the Actinides, A. J. Freeman, G. H. Lander, Eds. (North-Holland, Amsterdam, 1984), vol. 1, pp. 153–269.

3. P. Söderlind, O. Eriksson, B. Johansson, J. M. Wills, A. M. Boring, Nature374, 524 (1995).

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