While the layered 122 iron arsenide superconductors are highly anisotropic, unconventional, and exhibit several forms of electronic orders that coexist or compete with superconductivity in different regions of their phase diagrams, we find in the absence of iron in the structure that the superconducting characteristics of the end member ${\mathrm{BaPd}}_2{\mathrm{As}}_2$ are surprisingly conventional. Here we report on complementary measurements of specific heat, magnetic susceptibility, resistivity measurements, Andreev spectroscopy, and synchrotron high pressure x-ray diffraction measurements supplemented with theoretical calculations for ${\mathrm{BaPd}}_2{\mathrm{As}}_2$. Its superconducting properties are completely isotropic as demonstrated by the critical fields, which do not depend on the direction of the applied field. Under the application of high pressure, $T_c$ is linearly suppressed, which is the typical behavior of classical phonon-mediated superconductors with some additional effect of a pressure-induced decrease in the electronic density of states and the electron-phonon coupling parameters. Structural changes in the layered ${\mathrm{BaPd}}_2{\mathrm{As}}_2$ have been studied by means of angle-dispersive diffraction in a diamond-anvil cell. At 12 GPa and 24.2 GPa we observed pressure induced lattice distortions manifesting as the discontinuity and, hence discontinuity in the Birch-Murnaghan equation of state. The bulk modulus is $B_0=40\left(6\right)$ GPa below 12 GPa and $B_0=142\left(3\right)$ GPa below 27.2 GPa.

• Received 17 November 2017
• Revised 26 March 2018

DOI:https://doi.org/10.1103/PhysRevB.97.134508