Ambient- and low-temperature synchrotron x-ray diffraction study of BaFe2As2 and CaFe2As2 at high pressures up to 56 GPa

R. Mittal, S. K. Mishra, S. L. Chaplot, S. V. Ovsyannikov, E. Greenberg, D. M. Trots, L. Dubrovinsky, Y. Su, Th. Brueckel, S. Matsuishi, H. Hosono, and G. Garbarino
Phys. Rev. B 83, 054503 – Published 9 February 2011

Abstract

We report on high-pressure powder synchrotron x-ray diffraction studies on MFe2As2 (M=Ba, Ca) over a range of temperatures and pressures up to about 56 GPa using a membrane diamond-anvil cell. Our data indicate a phase transition to a collapsed tetragonal phase in both compounds upon compression. The data at 300 K are measured in both pressure-increasing and -decreasing cycles. Our measurements show that at 300 K in the Ba compound, the transition occurs at 27 GPa, which is much higher than the transition pressure of 1.7 GPa in the Ca compound. At low temperature, we could obtain data only in the pressure-increasing cycle, therefore a precise transition pressure is not identified. At a low temperature of 33 K, the transition to the tetragonal phase in the Ba compound starts, upon compression, at about 29 GPa, which is much higher than the transition pressure of 0.3 GPa at 40 K as known in the case of the Ca compound. The much higher transition pressure in the Ba compound may be due to its larger unit-cell volume at ambient pressure. It is important to note that the transition in both compounds occurs when they are compressed to almost the same value of the unit-cell volume and attain similar ct/at ratios. We also show that the FeAs4 tetrahedra are much less compressible and more distorted in the collapsed tetragonal phase than their nearly regular shape in the ambient pressure phase. We present a detailed analysis of the pressure dependence of the structures as well as equations of state in these important BaFe2As2 and CaFe2As2 compounds.

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  • Received 14 July 2010

DOI:https://doi.org/10.1103/PhysRevB.83.054503

©2011 American Physical Society

Authors & Affiliations

R. Mittal1, S. K. Mishra1, S. L. Chaplot1, S. V. Ovsyannikov2, E. Greenberg2,3, D. M. Trots2, L. Dubrovinsky2, Y. Su4, Th. Brueckel4,5, S. Matsuishi6, H. Hosono6, and G. Garbarino7

  • 1Solid State Physics Division, Bhabha Atomic Research Centre, Trombay, Mumbai 400 085, India
  • 2Bayerisches Geoinstitut, University Bayreuth, Universitatsstrasse 30, D-95440 Bayreuth, Germany
  • 3School of Physics and Astronomy, Tel-Aviv University, Israel
  • 4Jülich Centre for Neutron Science, IFF, Forschungszentrum Jülich, Outstation at FRM II, Lichtenbergstrasse 1, D-85747 Garching, Germany
  • 5Institut für Festkörperforschung, Forschungszentrum Jülich, D-52425 Jülich, Germany
  • 6Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan
  • 7European Synchrotron Radiation Facility, Boîte Postale 220, F-38043 Grenoble, France

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Vol. 83, Iss. 5 — 1 February 2011

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