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

被引:27
作者
Kacmarcik, J. [1 ,2 ,3 ]
Marcenat, C. [1 ]
Klein, T. [4 ,5 ,6 ]
Pribulova, Z. [2 ,3 ,4 ]
van der Beek, C. J. [7 ,8 ]
Konczykowski, M. [7 ,8 ]
Budko, S. L. [9 ,10 ]
Tillman, M. [9 ,10 ]
Ni, N. [9 ,10 ]
Canfield, P. C. [9 ,10 ]
机构
[1] CEA, Inst Nanosci & Cryogenie, SPSMS, LATEQS, F-38054 Grenoble 9, France
[2] Ctr Low Temp Phys IEP SAS, Kosice 04353, Slovakia
[3] FS UPJS, Kosice 04353, Slovakia
[4] CNRS, Inst Neel, F-38042 Grenoble 9, France
[5] Inst Univ France, F-38041 Grenoble 9, France
[6] Univ Grenoble 1, F-38041 Grenoble 9, France
[7] Ecole Polytech, CNRS, UMR7642, Solides Irradies Lab, F-91128 Palaiseau, France
[8] CCEA DSM IRAMIS, F-91128 Palaiseau, France
[9] Iowa State Univ, Dept Phys & Astron, Ames, IA 50011 USA
[10] Iowa State Univ, Ames Lab, Ames, IA 50011 USA
关键词
barium compounds; effective mass; Landau levels; magnetisation; mixed state; neodymium compounds; phase diagrams; potassium compounds; specific heat; superconducting critical field; superconducting materials; MAGNETIZATION; SUPERCONDUCTORS; FLUCTUATIONS;
D O I
10.1103/PhysRevB.80.014515
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
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 (C-p) 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 C-p 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 (gamma similar to 2.5) than in Nd(F,O)FeAs (gamma similar to 7.5).
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页数:7
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