Abstract:
A composite Cd$_{0.95}$Ni$_{0.05}$Sb crystal consisting of CdSb and NiSb inclusions was obtained by the modified Bridgman method. It was shown by the methods of scanning electron microscopy, X-ray phase analysis, energy-dispersive X-ray spectroscopy, and studies of Raman spectra, that the main CdSb matrix was a block single crystal (orthorhombic Pbca structure) containing microcrystalline acicular inclusions of the second NiSb phase (hexagonal structure of the NiAs type $P6_3/mmc$). It has been found that the anisotropy of single-crystal NiSb needles in samples of the Cd$_{0.95}$Ni$_{0.05}$Sb crystalline composite (needles are directed along and across the current direction) significantly affects the resistance and magnetoresistance of the crystal. The interface is a needle-like inclusion – the matrix can become superconducting, which affects the conductivity of the composite as a whole. However, this superconductivity is insufficient for the transition at the experimental temperatures to the superconducting phase with zero resistance of the composite.
Keywords:cadmium antimonide, nickel antimonide, composite, anisotropy of conductivity, interface superconductivity.