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Nodeless superconductivity in the presence of spin-density wave in pnictide superconductors: The case of BaFe2−xNixAs2

Mahmoud Abdel-Hafiez, Yuanyuan Zhang, Zheng He, Jun Zhao, Christoph Bergmann, Cornelius Krellner, Chun-Gang Duan, Xingye Lu, Huiqian Luo, Pengcheng Dai, Xiao-Jia Chen

DOI 10.1103/PhysRevB.91.024510 · Physical Review B

T1

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Abstract

The characteristics of Fe-based superconductors are manifested in their electronic, magnetic properties, and pairing symmetry of the Cooper pair, but the latter remain to be explored. Usually in these materials, superconductivity coexists and competes with magnetic order, giving unconventional pairing mechanisms. We report on the results of the bulk magnetization measurements in the superconducting state and the low-temperature specific heat down to 0.4 K for BaFe2−xNixAs2 single crystals. The electronic specific heat displays a pronounced anomaly at the superconducting transition temperature and a small residual part at low temperatures in the superconducting state. The normal-state Sommerfeld coefficient increases with Ni doping for x=0.092, 0.096, and 0.10, which illustrates the competition between magnetism and superconductivity. Our analysis of the temperature dependence of the superconducting-state specific heat and the London penetration depth provides strong evidence for a two-band s-wave order parameter. Further, the data of the London penetration depth calculated from the lower critical field follow an exponential temperature dependence, characteristic of a fully gapped superconductor. These observations clearly show that the superconducting gap in the nearly optimally doped compounds is nodeless.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
BaFe2-xNixAs2

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7.7Pressure unresolvedonset
BaFe2-xNixAs2

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18.5Pressure unresolvedonset
BaFe2-xNixAs2

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19Pressure unresolvedonset
BaFe2-xNixAs2

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20Pressure unresolvedonset
BaFe2-xNixAs2

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13.9Pressure unresolvedonset
BaFe1.90Ni0.10As2

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—Pressure unresolvedunknown
BaFe1.8Co0.2As2

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—Pressure not reportedunknown
Ba1-xKxFe2As2

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—Pressure not reportedunknown
Ba(Fe1-xCox)2As2

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—Pressure not reportedunknown
NaFe1-xCoxAs

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—Pressure not reportedunknown
LiFeAs

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—Pressure not reportedunknown
Ba0.6K0.4Fe2As2

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—Pressure not reportedunknown
FeSe

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—Pressure not reportedunknown
Ca0.32Na0.68Fe2As2

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—Pressure not reportedunknown
NdFeAsO0.82F0.18

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—Pressure not reportedunknown
LaFePO

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—Pressure not reportedunknown

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