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Saparov B, Cantoni C, Pan M, et al. Complex structures of different CaFe2As2 samples. Sci Rep. 2014;4:4120doi: 10.1038/srep04120.
Saparov, B., Cantoni, C., Pan, M., Hogan, T. C., Ratcliff, W., Wilson, S. D., Fritsch, K., Gaulin, B. D., Sefat, A. S., & Tachibana, M. (2014). Complex structures of different CaFe2As2 samples. Scientific reports, 44120. https://doi.org/10.1038/srep04120
Saparov, Bayrammurad, et al. "Complex structures of different CaFe2As2 samples." Scientific reports vol. 4 (2014): 4120. doi: https://doi.org/10.1038/srep04120
Saparov B, Cantoni C, Pan M, Hogan TC, Ratcliff W, Wilson SD, Fritsch K, Gaulin BD, Sefat AS, Tachibana M. Complex structures of different CaFe2As2 samples. Sci Rep. 2014 Feb 18;4:4120. doi: 10.1038/srep04120. PMID: 24844399; PMCID: PMC4027857.
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Sci Rep. 2014 Feb 18;4:4120. doi: 10.1038/srep04120.

Complex structures of different CaFe2As2 samples.

Scientific reports

Bayrammurad Saparov, Claudia Cantoni, Minghu Pan, Thomas C Hogan, William Ratcliff, Stephen D Wilson, Katharina Fritsch, Bruce D Gaulin, Athena S Sefat, Makoto Tachibana

Affiliations

  1. Material Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA.
  2. Department of Physics, Boston College, Chestnut Hill, MA 02467, USA.
  3. NIST Center for Neutron Research, Gaithersburg, MD 20899-6102, USA.
  4. Department of Physics and Astronomy, McMaster University, Hamilton, Ontario L8S 4M1, Canada.
  5. 1] Department of Physics and Astronomy, McMaster University, Hamilton, Ontario L8S 4M1, Canada [2] Brockhouse Institute for Materials Research, McMaster University, Hamilton, Ontario L8S 4M1, Canada [3] Canadian Institute for Advanced Research, 180 Dundas St W, Toronto, Ontario M5G 1Z8, Canada.

PMID: 24844399 PMCID: PMC4027857 DOI: 10.1038/srep04120

Abstract

The interplay between magnetism and crystal structures in three CaFe2As2 samples is studied. For the nonmagnetic quenched crystals, different crystalline domains with varying lattice parameters are found, and three phases (orthorhombic, tetragonal, and collapsed tetragonal) coexist between TS=95 K and 45 K. Annealing of the quenched crystals at 350°C leads to a strain relief through a large (~1.3%) expansion of the c-parameter and a small (~0.2%) contraction of the a-parameter, and to local ~0.2 Å displacements at the atomic-level. This annealing procedure results in the most homogeneous crystals for which the antiferromagnetic and orthorhombic phase transitions occur at TN/TS=168(1) K. In the 700°C-annealed crystal, an intermediate strain regime takes place, with tetragonal and orthorhombic structural phases coexisting between 80 to 120 K. The origin of such strong shifts in the transition temperatures are tied to structural parameters. Importantly, with annealing, an increase in the Fe-As length leads to more localized Fe electrons and higher local magnetic moments on Fe ions. Synergistic contribution of other structural parameters, including a decrease in the Fe-Fe distance, and a dramatic increase of the c-parameter, which enhances the Fermi surface nesting in CaFe2As2, are also discussed.

References

  1. J Am Chem Soc. 2008 Mar 19;130(11):3296-7 - PubMed
  2. Phys Rev Lett. 2008 Sep 5;101(10):107006 - PubMed
  3. Phys Rev Lett. 2008 Sep 12;101(11):117004 - PubMed
  4. Nat Mater. 2011 Sep 18;10(12):932-5 - PubMed

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