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Using four different experimental techniques, we performed comprehensive studies of the bulk superconductive properties of single crystals of the nearly optimally doped $Ba_{1-x}K_xFe_2As_2$ ($T_{c} approx 36,K$), a typical representative of the 122 family. We investigated temperature dependencies of the (i) specific heat $C_{el}(T)$, (ii) first critical magnetic field $H_{c1}(T)$, (iii) intrinsic multiple Andreev reflection effect (IMARE), and (iv) infrared reflectivity spectra. All data clearly show the presence of (at least) two superconducting nodeless gaps. The quantitative data on the superconducting spectrum obtained by four different techniques are consistent with each other: (a) the small energy gap $Delta_S(0) approx 1.8 - 2.5,meV$, and the large gap energy $Delta_L(0) approx 9.5 - 11.3,meV$ that demonstrates the signature of an extended s-wave symmetry ($sim~33 %$ in-plane anisotropy), (b) the characteristic ratio $2Delta_L/k_BT_C$ noticeably exceeds the BCS value.
We generalize the Chebyshev-Bogoliubov-deGennes method to treat multi-band systems to address the temperature dependence of the superconducting (SC) gaps of iron based superconductors. Four SC gaps associated with different electron and hole pockets
The precise momentum dependence of the superconducting gap in the iron-arsenide superconductor with Tc = 32K (BKFA) was determined from angle-resolved photoemission spectroscopy (ARPES) via fitting the distribution of the quasiparticle density to a m
We studied nearly optimally Ni-substituted BaFe$_{2-x}$Ni$_x$As$_2$ (BFNA) single crystals with $T_C approx 18.5$,K. In irreversible magnetization measurements, we determined the field dependence of the critical-current density and discuss the nature
We performed optical spectroscopy measurement on a superconducting Ba$_{0.6}$K$_{0.4}$Fe$_2$As$_2$ single crystal with T$_c$=37 K. Formation of the superconducting energy gaps in the far-infared reflectance spectra below T$_c$ is clearly observed. Th
We investigate the iron-based superconductor Ba$_{1-x}$K$_x$Fe$_2$As$_2$ using a terahertz (THz) pump near-infrared probe scheme. In the superconducting state we observe an instantaneous signal that is assigned to a non-linear THz Kerr effect. The TH