@article{oai:kyutech.repo.nii.ac.jp:00005860, author = {Abdel-Hafiez, M. and Zhao, Y. and Huang, Z. and Cho, C.-w. and Wong, C. H. and Hassen, A. and Ohkuma, M. and Fang, Y.-W. and Pan, B.-J. and Ren, Z.-A. and Sadakov, A. and Usoltsev, A. and Pudalov, V. and Mito, Masaki and 美藤, 正樹 and Lortz, R. and Krellner, C. and Yang, W.}, issue = {13}, journal = {Physical Review B}, month = {Apr}, note = {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 endmember BaPd2As2 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 BaPd2As2. 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, Tc is linearly suppressed, which is the typical behavior of classical phononmediated 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 layeredBaPd2As2 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 B0 = 40(6) GPa below 12 GPa and B0 = 142(3) GPa below 27.2 GPa.}, pages = {134508-1--134508-9}, title = {High-pressure effects on isotropic superconductivity in the iron-free layered pnictide superconductor BaPd2As2}, volume = {97}, year = {2018}, yomi = {ミトウ, マサキ} }