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Superconducting specific heat jump $��C_{\rm el} \propto T_c^��\ (��\approx 2)$ for K$_{1-x}$Na$_x$Fe$_2$As$_2$

Authors :
Grinenko, V.
Efremov, D. V.
Drechsler, S. -L.
Aswartham, S.
Gruner, D.
Roslova, M.
Morozov, I.
Nenkov, K.
Wurmehl, S.
Wolter, A. U. B.
Holzapfel, B.
B��chner
Publication Year :
2013
Publisher :
arXiv, 2013.

Abstract

We present a systematic study of the electronic specific heat jump ($��C_{\rm el}$) at the superconducting transition temperature $T_c$ of K$_{1-x}$Na$_x$Fe$_2$As$_2$. Both $T_c$ and $��C_{\rm el}$ monotonously decrease with increasing $x$. The specific heat jump scales approximately with a power-law, $��C_{\rm el} \propto T_c^��$, with $��\approx 2$ determined by the impurity scattering rate, in contrast to most iron-pnictide superconductors, where the remarkable Bud'ko-Ni-Canfield (BNC) scaling $��C_{\rm el} \propto T^3$ has been found. Both the $T$ dependence of $C_{\rm el}(T)$ in the superconducting state and the nearly quadratic scaling of $��C_{\rm el}$ at $T_c$ are well described by the Eliashberg-theory for a two-band $d$-wave superconductor with weak pair-breaking due to nonmagnetic impurities. The disorder induced by the Na substitution significantly suppresses the small gaps leading to gapless states in the slightly disordered superconductor, which results in a large observed residual Sommerfeld coefficient in the superconducting state for $x > 0$.<br />5 pages, 3 figures, and supplement

Details

Database :
OpenAIRE
Accession number :
edsair.doi...........ae9ff2975c512e9b607606ccc55fa3fd
Full Text :
https://doi.org/10.48550/arxiv.1308.2201