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Phys. Rev. B 78, 014507 (2008) [9 pages]

Anisotropic thermodynamic and transport properties of single-crystalline Ba1−xKxFe2As2 (x=0 and 0.45)

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N. Ni1,2, S. L. Bud’ko1,2, A. Kreyssig1,2, S. Nandi1,2, G. E. Rustan1,2, A. I. Goldman1,2, S. Gupta1,3, J. D. Corbett1,3, A. Kracher1, and P. C. Canfield1,2
1Ames Laboratory US DOE, Iowa State University, Ames, Iowa 50011, USA
2Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
3Department of Chemistry, Iowa State University, Ames, Iowa 50011, USA

Received 11 June 2008; revised 18 June 2008; published 10 July 2008

See accompanying Physics Synopsis

Single crystals of BaFe2As2 and Ba0.55K0.45Fe2As2 have been grown out of excess Sn with 1% or less incorporation of solvent. The crystals are exceptionally micaceous, are easily exfoliated, and can have dimensions as large as 3×3×0.2 mm3. The BaFe2As2 single crystals manifest a structural phase transition from a high-temperature tetragonal phase to a low-temperature orthorhombic phase near 85 K and do not show any sign of superconductivity down to 1.8 K. This transition can be detected in the electrical resistivity, Hall resistivity, specific heat, and the anisotropic magnetic susceptibility. In the Ba0.55K0.45Fe2As2 single crystals this transition is suppressed and instead superconductivity occurs with a transition temperature near 30 K. Whereas the superconducting transition is easily detected in resistivity and magnetization measurements, the change in specific heat near Tc is small, but resolvable, giving ΔCp/γTc≈1. The application of a 140 kOe magnetic field suppresses Tc by only ∼4 K when applied along the c axis and by ∼2 K when applied perpendicular to the c axis. The ratio of the anisotropic upper critical fields, γ=Hc2c/Hc2c, varies between 2.5 and 3.5 for temperatures down to ∼2 K below Tc.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.78.014507
DOI:
10.1103/PhysRevB.78.014507
PACS:
74.70.Dd, 74.25.Op, 61.50.Ks, 65.40.Ba