d-metal oxides play a crucial role in numerous technological applications and show a great variety of magnetic properties. We have systematically investigated the structural properties, magnetic ground states, and fundamental electronic properties of 100 binary d-metal oxides using hybrid density functional methods and localized basis sets composed of Gaussian-type functions. The calculated properties are compared with experimental information in all cases where experimental data are available. The used PBE0 hybrid density functional method describes the structural properties of the studied d-metal oxides well, except in the case of molecular oxides with weak intermolecular forces between the molecular units. Empirical D3 dispersion correction does not improve the structural description of the molecular oxides. We provide a database of optimized geometries and magnetic ground states to facilitate future studies on the more complex properties of the binary d-metal oxides.
We
obtained single crystals of the binary mixed-valent fluorides Mn2F5 and Mn3F8 using a high-pressure/high-temperature
approach. Mn2F5 crystallizes isotypic to CaCrF5 in the monoclinic space group C2/c (No. 15), with a = 8.7078(8) Å, b = 6.1473(6) Å, c = 7.7817(7) Å,
β = 117.41(1)°, V = 369.80(6) Å3, Z = 4, and mC28 at T = 173 K. Mn3F8 crystallizes in the
monoclinic space group P21 (No. 4) with a = 5.5253(2) Å, b = 4.8786(2) Å, c = 9.9124(4) Å, β = 92.608(2)°, V = 266.92(2) Å3, Z = 2,
and mP22 at T = 183 K and presents
a new structure type. Crystal-chemical reasoning, CHARDI calculations,
and quantum-chemical calculations allowed for the assignment of the
oxidation states of the Mn atoms. In both bulk compounds, MnF2 was present as an impurity, as evidenced by powder X-ray
diffraction and IR and Raman spectroscopy.
BrF 5 can be prepared by treating BrF 3 with fluorine under UV light in the region of 300 to 400 nm at room temperature. It was analyzed by UV-Vis, NMR, IR and Raman spectroscopy. Its crystal structure was redetermined by X-ray diffraction, and its space group was corrected to Pnma. Quantum-chemical calculations were performed for the band assignment of the vibrational spectra. A monoclinic polymorph of BrF 5 was quantum chemically predicted and then observed as its low-temperature modification in space group P2 1 /c by single crystal X-ray diffraction. BrF 5 reacts with the alkali metal fluorides AF (A = K, Rb) to form alkali metal hexafluoridobromates(V), A[BrF 6 ] the crystal structures of which have been determined. Both compounds crystallize in the K[AsF 6 ] structure type (R � 3, no. 148, hR24). For the species [BrF 6 ] + , BrF 5 , [BrF 6 ] À , and [IF 6 ] À , the chemical bonds and lone pairs on the heavy atoms were investigated by means of intrinsic bond orbital analysis.
Solid gold(I) fluoride remains as an unsynthesized and uncharacterized compound. We have performed a search for potential gold(I) fluoride crystal structures using USPEX evolutionary algorithm and dispersion‐corrected hybrid density functional methods. Over 4000 AuF crystal structures have been investigated. Behavior of the AuF crystal structures under pressure was studied up to 25 GPa, and we also evaluated the thermodynamic stability of the hypothetical AuF crystal structures with respect to AuF3, AuF5, and Au3F8. Mixed‐valence compound Au3[AuF4] with Au atoms in various formal oxidation states emerged as the thermodynamically most stable AuF species.
A search was made for an electron-positron pair transition from the 10.98-Mev 0~ state of O 16 to the 0 + ground state using the F 19 (^,G!)0 16 * reaction and an intermediate-image pair spectrometer. No 10.98-Mev pairs were observed with an intensity as great as 2X 10~5 that of the 3.86 Mev Ml cascade gamma-ray from the 10.98-Mev to the 7.12-Mev 1" state. This result suggests a lower limit of r>2XlO~8 sec for the partial lifetime of a 10.98-Mev 0~->0 + pair transition.
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