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CONDENSED MATTER
Determination of the superconducting order parameter of BaFe$_{1.92}$Ni$_{0.08}$As$_2$ weakly underdoped pnictides by two complementary techniques
A. V. Sadakova,
A. V. Muratova,
S. A. Kuzmichevab,
O. A. Sobolevskiya,
B. I. Massalimova,
A. R. Prishchepaa,
V. M. Mikhailova,
K. S. Pervakova,
V. A. Vlasenkoa,
T. E. Kuzmichevaa a Lebedev Physical Institute, Russian Academy of Sciences, Moscow, 119991 Russia
b Faculty of Physics, Moscow State University, Moscow, 119991 Russia
Abstract:
The structure of the superconducting order parameter of weakly underdoped BaFe
$_{1.92}$Ni
$_{0.08}$As
$_2$ pnictides with the critical temperature
$T_c \approx 18.2$ K has been determined. Two microscopic superconducting order parameters — the small superconducting gap
$\Delta_S(0)$ and, supposedly, the edges of the large gap with anisotropy in the
$ab$ plane
$\Delta_L^{\rm out}(0)$ and
$\Delta_L^{\rm in}(0)$ — have been determined at
$T \ll T_c$, together with their temperature dependences, using incoherent multiple Andreev reflection spectroscopy. It has been shown that the determined temperature dependence of the lower critical field
$H_{c1}(T)$ can be described in the two-band approximation both within the so-called alpha model (using experimental
$\Delta_S(0)$,
$\Delta_L^{\rm out}(0)$, and
$\Delta_L^{\rm in}(0)$ values) and using the temperature dependences
$\Delta_S(T)$ and
$\Delta_L^{\rm out,in}(T)$ obtained by multiple Andreev reflection spectroscopy under the assumption of a fairly strong anisotropy of the small superconducting gap, where the experimental
$\Delta_S(0)$ value is taken as the outer edge of its angular distribution.
Received: 29.07.2022
Revised: 28.09.2022
Accepted: 28.09.2022
DOI:
10.31857/S1234567822220074