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Phys. Rev. B 80, 014515 (2009) [7 pages]

Strongly dissimilar vortex-liquid regimes in single-crystalline NdFeAs(O,F) and (Ba,K)Fe2As2: A comparative study

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J. Kacmarcik1,2, C. Marcenat1, T. Klein3,4, Z. Pribulova2,3, C. J. van der Beek5, M. Konczykowski5, S. L. Budko6, M. Tillman6, N. Ni6, and P. C. Canfield6
1CEA, Institut Nanosciences et Cryogénie, SPSMS–LATEQS, 17 rue des Martyrs, 38054 Grenoble Cedex 9, France
2Centre of Low Temperature Physics IEP SAS and FS UPJŠ, Watsonova 47, 043 53 Košice, Slovakia
3Institut Néel, CNRS, B.P. 166, 38042 Grenoble Cedex 9, France
4Institut Universitaire de France and Université Joseph Fourier, B.P. 53, 38041 Grenoble Cedex 9, France
5Laboratoire des Solides Irradiés, Ecole Polytechnique, CNRS UMR7642 and CCEA/DSM/IRAMIS, 91128 Palaiseau, France
6Department of Physics & Astronomy and Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA

Received 29 January 2009; revised 30 June 2009; published 21 July 2009

The extent of the vortex-liquid state in underdoped single crystals of the oxypnictide superconductors NdFeAs(O,F) and (Ba,K)Fe2As2 is investigated using specific heat (Cp) and Hall-probe magnetization experiments. In both materials, the vortex liquid lies entirely in the regime where the three-dimensional lowest Landau-level (3D-LLL) approximation is valid and both systems present a very small shift in the specific heat anomaly with increasing field. The irreversibility line, defined as the onset of diamagnetic response, is very rapidly shifted toward lower temperatures in NdFeAs(O,F) but remains close to the Cp anomaly in (Ba,K)Fe2As2. These measurements strongly suggest that a vortex-liquid phase occupies a large portion of the mixed-state phase diagram of NdFeAs(O,F) but not in (Ba,K)Fe2As2. This difference can be attributed to different Ginzburg numbers Gi, the latter being about 100 times larger in NdFeAs(O,F) than in (Ba,K)Fe2As2. The angular dependence of the upper critical field, derived from 3D-LLL scaling of the irreversibility lines, presents deviations from the standard 3D effective-mass model in both materials with an anisotropy being about three times smaller in (Ba,K)Fe2As2 (γ∼2.5) than in Nd(F,O)FeAs (γ∼7.5).

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.80.014515
DOI:
10.1103/PhysRevB.80.014515
PACS:
74.25.Ha, 74.25.Fy, 74.25.Nf, 74.25.Op