La₃BaSi₅N₉O₂:Ce³⁺ – A Yellow Phosphor with an Unprecedented Tetrahedra Network Structure Investigated by Combination of Electron Microscopy and Synchrotron X‑ray Diffraction

Due to the relationship between structure and luminescence properties, detailed crystal structure determination for microcrystalline phosphors is necessary for a profound understanding of materials properties. The yellow phosphor La₃BaSi₅N₉O₂:Ce³⁺ (λ_max = 578 nm; fwhm ∼4700 cm^–1) was characterized by a combination of transmission electron microscopy (TEM) and synchrotron microfocus diffraction as only agglomerates of crystals with a maximum size of a few μm could be obtained yet. La₃BaSi₅N₉O₂:Ce³⁺ was synthesized from LaF₃, La­(NH₂)₃, BaH₂, Si­(NH)₂, and CeF₃ in a radio frequency furnace. It crystallizes in space group <i>Pmn</i>2₁ (no. 31) with <i>a</i> = 9.5505(8), <i>b</i> = 19.0778(16), <i>c</i> = 12.1134(9) Å, and <i>Z</i> = 8. Its interrupted three-dimensional tetrahedra network contains <i>zehner</i> and <i>dreier</i> rings of vertex-sharing SiN₄ and SiN₂O₂ tetrahedra. The crystal structure was confirmed by high-resolution TEM and Z-contrast scanning TEM. The element distribution was derived by bond-valence sum calculations. The infrared spectrum proves the absence of N–H bonds

La₃BaSi₅N₉O₂:Ce³⁺ – A Yellow Phosphor with an Unprecedented Tetrahedra Network Structure Investigated by Combination of Electron Microscopy and Synchrotron X‑ray Diffraction

Due to the relationship between structure and luminescence properties, detailed crystal structure determination for microcrystalline phosphors is necessary for a profound understanding of materials properties. The yellow phosphor La₃BaSi₅N₉O₂:Ce³⁺ (λ_max = 578 nm; fwhm ∼4700 cm^–1) was characterized by a combination of transmission electron microscopy (TEM) and synchrotron microfocus diffraction as only agglomerates of crystals with a maximum size of a few μm could be obtained yet. La₃BaSi₅N₉O₂:Ce³⁺ was synthesized from LaF₃, La­(NH₂)₃, BaH₂, Si­(NH)₂, and CeF₃ in a radio frequency furnace. It crystallizes in space group <i>Pmn</i>2₁ (no. 31) with <i>a</i> = 9.5505(8), <i>b</i> = 19.0778(16), <i>c</i> = 12.1134(9) Å, and <i>Z</i> = 8. Its interrupted three-dimensional tetrahedra network contains <i>zehner</i> and <i>dreier</i> rings of vertex-sharing SiN₄ and SiN₂O₂ tetrahedra. The crystal structure was confirmed by high-resolution TEM and Z-contrast scanning TEM. The element distribution was derived by bond-valence sum calculations. The infrared spectrum proves the absence of N–H bonds

Puzzling Intergrowth in Cerium Nitridophosphate Unraveled by Joint Venture of Aberration-Corrected Scanning Transmission Electron Microscopy and Synchrotron Diffraction

Thorough investigation of nitridophosphates has rapidly accelerated through development of new synthesis strategies. Here we used the recently developed high-pressure metathesis to prepare the first rare-earth metal nitridophosphate, Ce₄Li₃P₁₈N₃₅, with a high degree of condensation >1/2. Ce₄Li₃P₁₈N₃₅ consists of an unprecedented hexagonal framework of PN₄ tetrahedra and exhibits blue luminescence peaking at 455 nm. Transmission electron microscopy (TEM) revealed two intergrown domains with slight structural and compositional variations. One domain type shows extremely weak superstructure phenomena revealed by atomic-resolution scanning TEM (STEM) and single-crystal diffraction using synchrotron radiation. The corresponding superstructure involves a modulated displacement of Ce atoms in channels of tetrahedra 6-rings. The displacement model was refined in a supercell as well as in an equivalent commensurate (3 + 2)-dimensional description in superspace group <i>P</i>6₃(α, β, 0)­0­(−α – β, α, 0)­0. In the second domain type, STEM revealed disordered vacancies of the same Ce atoms that were modulated in the first domain type, leading to sum formula Ce_{4–0.5<i>x</i>}Li₃P₁₈N_{35–1.5<i>x</i>}O_1.5<i>x</i> (<i>x</i> ≈ 0.72) of the average structure. The examination of these structural intricacies may indicate the detection limit of synchrotron diffraction and TEM. We discuss the occurrence of either Ce displacements or Ce vacancies that induce the incorporation of O as necessary stabilization of the crystal structure