Superconductivity and phase diagrams of CaK(Fe$_{1-x}$Mn$_{x}$)$_{4}$As$_{4}$ single crystals

M. Xu; J. Schmidt; E. Gati; L. Xiang; W. R. Meier; V. G. Kogan; S. L. Bud'ko; P. C. Canfield

doi:10.1103/PhysRevB.105.214526

paper

Superconductivity and phase diagrams of CaK(Fe $_{1 - x}$ Mn $_{x}$ ) $_{4}$ As $_{4}$ single crystals

arXiv:2204.10925 · doi:10.1103/PhysRevB.105.214526

Abstract

Members of the CaK(Fe $_{1 - x}$ Mn $_{x}$ ) $_{4}$ As $_{4}$ series have been synthesized in single crystalline form and characterized by elemental analysis, thermodynamic and transport measurements. These measurements show that the superconducting transition temperature decreases monotonically and is finally suppressed below 1.8 K. For $x$ -values greater than 0.016, signatures of a magnetic transition can be detected in both thermodynamic and transport measurements in which kink-like features allow for the determination of the transition temperature, $T^{*}$ , that increases as Mn substitution increases. A temperature-composition ( $T$ - $x$ ) phase diagram is constructed, revealing a half-dome of superconductivity with the magnetic transition temperature, $T^{*}$ , appearing near 26 K for $x$ $\sim$ 0.017 and rising slowly up to 33 K for $x$ $\sim$ 0.036. Specific heat data are used to track the jump in specific heat at $T_{c}$ ; The CaK(Fe $_{1 - x}$ Mn $_{x}$ ) $_{4}$ As $_{4}$ data does not follow the scaling of $Δ$ $C_{p}$ with $T_{c}^{3}$ as many of the other Fe-based superconducting systems do. Elastoresistivity coefficients, $2 m_{66}$ and $m_{11} - m_{12}$ , as a function of temperature are also measured. $2 m_{66}$ and $m_{11} - m_{12}$ are qualitatively similar to CaK(Fe $_{1 - x}$ Ni $_{x}$ ) $_{4}$ As $_{4}$ . This may indicate that the magnetic order in Mn substituted system may be still the same as CaK(Fe $_{1 - x}$ Ni $_{x}$ ) $_{4}$ As $_{4}$ . A clear change in $H_{c 2}^{'}$ ( $T$ )/ $T_{c}$ , where $H_{c 2}^{'}$ ( $T$ ) is d $H_{c 2}$ ( $T$ )/d $T$ , at $x$ $\sim$ 0.015 is observed and probably is related to change of the Fermi surface due to magnetic order. Coherence lengths and the London penetration depths are also calculated based on $H_{c 1}$ and $H_{c 2}$ data. Coherence lengths as the function of $x$ also shows the changes near $x$ = 0.015.

Fig. 16 a and b were corrected

Superconductivity and phase diagrams of CaK(Fe $_{1 - x}$ Mn $_{x}$ ) $_{4}$ As $_{4}$ single crystals

Abstract

References in corpus (7)

Cited by in corpus (7)

Superconductivity and phase diagrams of CaK(Fe1−x​Mnx​)4​As4​ single crystals

Abstract

References in corpus (7)

Cited by in corpus (7)

Superconductivity and phase diagrams of CaK(Fe $_{1 - x}$ Mn $_{x}$ ) $_{4}$ As $_{4}$ single crystals