TY - JOUR
T1 - Anisotropic thermodynamic and transport properties of single-crystalline CaKFe4As4
AU - Meier, W. R.
AU - Kong, T.
AU - Kaluarachchi, U. S.
AU - Taufour, V.
AU - Jo, N. H.
AU - Drachuck, G.
AU - Böhmer, A. E.
AU - Saunders, S. M.
AU - Sapkota, A.
AU - Kreyssig, A.
AU - Tanatar, M. A.
AU - Prozorov, R.
AU - Goldman, A. I.
AU - Balakirev, Fedor F.
AU - Gurevich, Alex
AU - Bud'Ko, S. L.
AU - Canfield, P. C.
N1 - Publisher Copyright:
© 2016 American Physical Society.
PY - 2016/8/1
Y1 - 2016/8/1
N2 - Single-crystalline, single-phase CaKFe4As4 has been grown out of a high-temperature, quaternary melt. Temperature-dependent measurements of x-ray diffraction, anisotropic electrical resistivity, elastoresistivity, thermoelectric power, Hall effect, magnetization, and specific heat, combined with field-dependent measurements of electrical resistivity and field and pressure-dependent measurements of magnetization indicate that CaKFe4As4 is an ordered, stoichiometric, Fe-based superconductor with a superconducting critical temperature, Tc=35.0±0.2 K. Other than superconductivity, there is no indication of any other phase transition for 1.8K≤T≤300 K. All of these thermodynamic and transport data reveal striking similarities to those found for optimally or slightly overdoped (Ba1-xKx)Fe2As2, suggesting that stoichiometric CaKFe4As4 is intrinsically close to what is referred to as "optimal-doped" on a generalized, Fe-based superconductor, phase diagram. The anisotropic superconducting upper critical field, Hc2(T), of CaKFe4As4 was determined up to 630 kOe. The anisotropy parameter γ(T)=Hc2/Hc2 , for H applied perpendicular and parallel to the c axis, decreases from ≃2.5 at Tc to ≃1.5 at 25 K, which can be explained by interplay of paramagnetic pair breaking and orbital effects. The slopes of dHc2 /dT≃-44 kOe/K and dHc2/dT≃-109 kOe/K at Tc yield an electron mass anisotropy of m/m ≃1/6 and short Ginzburg-Landau coherence lengths ξ (0)≃5.8Å and ξ(0)≃14.3Å. The value of Hc2(0) can be extrapolated to ≃920 kOe, well above the BCS paramagnetic limit.
AB - Single-crystalline, single-phase CaKFe4As4 has been grown out of a high-temperature, quaternary melt. Temperature-dependent measurements of x-ray diffraction, anisotropic electrical resistivity, elastoresistivity, thermoelectric power, Hall effect, magnetization, and specific heat, combined with field-dependent measurements of electrical resistivity and field and pressure-dependent measurements of magnetization indicate that CaKFe4As4 is an ordered, stoichiometric, Fe-based superconductor with a superconducting critical temperature, Tc=35.0±0.2 K. Other than superconductivity, there is no indication of any other phase transition for 1.8K≤T≤300 K. All of these thermodynamic and transport data reveal striking similarities to those found for optimally or slightly overdoped (Ba1-xKx)Fe2As2, suggesting that stoichiometric CaKFe4As4 is intrinsically close to what is referred to as "optimal-doped" on a generalized, Fe-based superconductor, phase diagram. The anisotropic superconducting upper critical field, Hc2(T), of CaKFe4As4 was determined up to 630 kOe. The anisotropy parameter γ(T)=Hc2/Hc2 , for H applied perpendicular and parallel to the c axis, decreases from ≃2.5 at Tc to ≃1.5 at 25 K, which can be explained by interplay of paramagnetic pair breaking and orbital effects. The slopes of dHc2 /dT≃-44 kOe/K and dHc2/dT≃-109 kOe/K at Tc yield an electron mass anisotropy of m/m ≃1/6 and short Ginzburg-Landau coherence lengths ξ (0)≃5.8Å and ξ(0)≃14.3Å. The value of Hc2(0) can be extrapolated to ≃920 kOe, well above the BCS paramagnetic limit.
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U2 - 10.1103/PhysRevB.94.064501
DO - 10.1103/PhysRevB.94.064501
M3 - Article
AN - SCOPUS:84982993853
SN - 2469-9950
VL - 94
JO - Physical Review B
JF - Physical Review B
IS - 6
M1 - 064501
ER -