Solving the “Coloring Problem” in InPd3–xAgx(x = 0–0.7) by Phase Diagrams Modeling and Diffraction Experiments

  • Nilanjan Roy
  • , Sandip K. Kuila
  • , Jin Li
  • , Mustafa Eid
  • , Kathryn MacIntosh
  • , Parna Pramanik
  • , Thomas Proffen
  • , Michael J. Janik
  • , Robert M. Rioux
  • , Partha Pratim Jana

Research output: Contribution to journalArticlepeer-review

Abstract

A series of InPd3–xAgx(x = 0–1) compositions were synthesized by conventional high-temperature synthesis, and as-synthesized samples were characterized by powder X-ray diffraction experiments. Up to x = 0.7, InPd3–xAgxadopts the ternary substitutional variant of the InPd3structure (TiAl3-type), when x > 0.7, elemental Ag starts to segregate along with the main phase. Accurate structural characterization in InPd3–xAgxfaces a critical challenge due to the narrow X-ray scattering contrast among constituents In, Pd, and Ag and nearly identical neutron scattering lengths of Pd and Ag. To overcome this “coloring problem”, a combination of calculation of phase diagrams modeling (CALPHAD) and diffraction techniques (X-ray and neutron) was employed. In the compositional range 0 ≤ x ≤ 0.7, InPd3–xAgxpresents a ternary variant of the TiAl3-type structure, where Ag atoms selectively substitute one (the 2b Wyckoff site) of the two Pd sites in InPd3. Notably, in contrast to the isologous InPd3–xCux(x = 0–1) system, Ag substitution does not form an ordered VRh2Sn-type structure at the limiting composition. The distinct site preference in InPd3–xAgxis elucidated by charge population analysis, electronic structure calculations, and orbital-resolved chemical bonding investigations, and the extent of substitution is supported by formation free energy calculations.

Original languageEnglish
Pages (from-to)23535-23545
Number of pages11
JournalInorganic Chemistry
Volume64
Issue number48
DOIs
StatePublished - Dec 8 2025

Funding

P.P.J. thanks the Science and Engineering Research Board (SERB), India (Grant CRG/2020004115), for financial support. S.K.K. and N.R. acknowledge CSIR for research fellowships. P.P. acknowledges the Prime Minister Research Fellowship (PMRF) for her research fellowship. A significant part of the material is based upon work supported partially by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Catalysis Division, under Grant DE-SC0020147. J.L. and M.J.J. acknowledge this U.S. Department of Energy (DOE) funding. The work of M.E. and R.M.R. was supported by the National Science Foundation under Grant CHE-2247797. A portion of this research used resources at the Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The beamtime was allocated to POWGEN on Proposal IPTS-36151.

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