Crystal structure, phase width, and physical properties of the barium tetrel selenides Ba6Si2−xGexSe12 (x = 0, 0.5, 1, and 1.5) with ultralow thermal conductivity

• Published in: Dalton transactions : an international journal of inorganic chemistry Vol. 52; no. 43; pp. 15831 - 15838
• Main Authors: Menezes, Luke T, Assoud, Abdeljalil, Kleinke, Holger
• Format: Journal Article
• Language: English
• Published: Cambridge Royal Society of Chemistry 07.11.2023
• Subjects: Absorption spectra; Barium; Crystal structure; Density functional theory; Energy gap; Germanium; Heat conductivity; Heat transfer; Lattice parameters; Lattice vibration; Light sources; Mathematical analysis; Physical properties; Raman spectra; Room temperature; Selenides; Selenium; Silicon; Stoichiometry; Thermal conductivity
• ISSN: 1477-9226; 1477-9234
• DOI: 10.1039/d3dt02516k

The new compound Ba6Si2Se12 was synthesized, and the crystal structure and physical properties are reported here. Ba6Si2Se12 adopts a new structure type in the triclinic P1 space group with the lattice parameters a = 9.1822(7) Å, b = 12.2633(14) Å, c = 12.3636(18) Å, α = 109.277(3)°, β = 104.734(2)°, and γ = 100.4067(16)°. Notably, the structure features disordered Se22− dumbbells that have also been observed in the germanium selenide with the analogous stoichiometry (Ba6Ge2Se12). Density functional theory calculations revealed that Ba6Si2Se12 is a semiconductor with a calculated band gap of 1.74 eV. UV/vis/NIR absorption spectra indicated that the experimental band gap of Ba6Si2Se12 is 1.89 eV. While exploring this compound's phase width, it was discovered that up to 75% of the Si could be substituted with Ge while retaining the structure type. Rietveld refinements were performed on the phase-pure samples of Ba6Si2−xGexSe12 (x = 0, 0.5, 1, and 1.5) using data collected at the Canadian Light Source's High Energy Wiggler Beamline. The cell parameters, Si/Ge occupancies, and disordered Se22− occupancies were studied. Raman spectra displayed the expected Si–Se and Ge–Se stretching modes from 215 cm−1 to 280 cm−1. The samples were also hot-pressed into pellets to determine their thermal conductivity values ranging from 0.5 to 0.4 W m−1 K−1 for the x = 0, 0.5, and 1.5 samples. The x = 1 sample stood out with a remarkably low thermal conductivity of 0.3 W m−1 K−1, consistent from room temperature up to 573 K.