Application of Quantum-Mechanical Methods to Simple Inorganic “Molecules” of Relevance to Mineralogy, and to Oxide Minerals

Author(s):  
John A. Tossell ◽  
David J. Vaughan

As noted in the introduction to this text, much can be learned through the application of both quantum-mechanical calculations and experimental techniques to simple molecules that contain bonds of the type found in the important groups of minerals. One reason for this approach is that calculations at a higher level of quantum-mechanical rigor can be applied to such simple systems. This approach will be illustrated with reference to the SiO, SiO2, Si2O2, Si3O3, and SiF4 molecules. Attention will then be turned to the major oxide minerals MgO, Al2O3, and SiO2 and the binary transition-metal oxides of Ti, Mn, and Fe, with some brief discussion of the series of transition-metal monoxides (MnO, FeO, CoO, NiO) and complex oxides (FeCr2O4, FeTiO3, etc.), and of the problem of the calculation of Mössbauer parameters in iron oxides (and other compounds). Although silicon monoxide, SiO, is not an important component of minerals, it is an important chemical constituent in interstellar and circumstellar space and an important starting material for the gas-phase synthesis of silicates from components of the nebula (Day and Donn, 1978). The structure, energetics, and spectral properties of SiO have been calculated by a number of different methods. The Si-O bond distance calculated using ab initio Hartree-Fock-Roothaan SCF methods at the 6-31G* basis- set level is 1.487 Å (Snyder and Raghavachari, 1984), slightly smaller than the experimental value of 1.5097 Å (Field et al., 1976). A near Hartree- Fock limit basis set and limited configuration-interaction calculation has given the slightly better value of 1.496 Å (Langhoff and Arnold, 1979). This study also gave a bond dissociation energy of 8.10 eV, compared to an experimental value of 8.26 ± 0.13 eV (Hildenbrand, 1972), and a bond stretching frequency of 1248 cm- 1 , compared to an experimental value of 1242 cm-1 (Anderson and Ogden, 1969). Even more highly correlated calculations give a bond distance of 1.515 Å and a stretching frequency of 1242 cm-1 (Werner et al., 1982). The 6-31G* basis-set Hartree-Fock-Roothaan calculation also gives an almost exactly correct bond-stretching frequency after the standard correction factor describing correlation effects is applied (Hehre et al., 1986).

2018 ◽  
Vol 25 (3) ◽  
pp. 899-905 ◽  
Author(s):  
Patric Zimmermann ◽  
Robert J. Green ◽  
Maurits W. Haverkort ◽  
Frank M. F. de Groot

Some initial instructions for theQuanty4RIXSprogram written in MATLAB®are provided. The program assists in the calculation of 1s 2p RIXS and 1s 2p RIXS–MCD spectra usingQuanty. Furthermore, 1s XAS and 2p 3d RIXS calculations in different symmetries can also be performed. It includes the Hartree–Fock values for the Slater integrals and spin–orbit interactions for several 3dtransition metal ions that are required to create the .lua scripts containing all necessary parameters and quantum mechanical definitions for the calculations. The program can be used free of charge and is designed to allow for further adjustments of the scripts.


2003 ◽  
Vol 81 (4) ◽  
pp. 275-283 ◽  
Author(s):  
Gang Wu ◽  
Alan Wong ◽  
Suning Wang

We report solid-state 25Mg NMR, X-ray crystallographic, and quantum-mechanical calculation results for bis(pyridine)(5,10,15,20-tetraphenylporphyrinato)magnesium(II), Mg(TPP)·Py2. Mg(TPP)·Py2 crystallizes in the triclinic form, in the space group P[Formula: see text]. The unit cell parameters are: a = 9.6139(13) Å, b = 11.0096(16) Å, c = 11.8656(15) Å; α = 102.063(3)°, β = 103.785(3)°, γ = 114.043(2)°; Z = 1. The Mg(II) ion is coordinated to four nitrogen atoms from the porphyrin ring and two nitrogen atoms from the axial pyridine ligands, forming a regular octahedron. The 25Mg quadrupole coupling constant (CQ) is 15.32 ± 0.02 MHz, which represents the largest value so far observed for 25Mg nuclei. The electric field gradient tensor at the Mg site is axially symmetric, ηQ = 0.00 ± 0.05. The 25Mg chemical shielding anisotropy is too small to be accurately determined. Quantum-mechanical calculations using a 6–31G(d) basis set reproduce reasonably well the observed 25Mg NMR data for Mg(TPP)·Py2. The calculations also suggest that the span of the 25Mg chemical shift tensor is less than 50 ppm. Using a theoretical approach, we also investigate the dependence of the 25Mg quadrupole coupling constant on the Mg—Nax bond distance. The calculation suggests that the 25Mg quadrupole coupling constant for an Mg(II) ion at the center of a porphyrin ring without axial ligands is approximately 22 MHz, which may be treated as an upper limit of the 25Mg quadrupole coupling constant for all Mg–porphyrin complexes.Key words: 25Mg NMR, crystal structure, quantum chemical calculation, quadrupole parameter, tetraphenylporphyrin.


2019 ◽  
Author(s):  
Qing Zhao ◽  
Heather Kulik

Approximate, semi-local density functional theory (DFT) suffers from delocalization error that can lead to a paradoxical overbinding of surface adsorbates and overestimation of surface stabilities in catalysis modeling. We investigate the effect of two widely applied approaches for delocalization error correction, i) affordable DFT+U (i.e., semi-local DFT augmented with a Hubbard U) and ii) hybrid functionals with an admixture of Hartree-Fock (HF) exchange, on surface and adsorbate energies across a range of rutile transition metal oxides widely studied for their promise as water splitting catalysts. We observe strongly row- and period-dependent trends with DFT+U, which increases surface formation energies only in early transition metals (e.g., Ti, V) and decreases adsorbate energies only in later transition metals (e.g., Ir, Pt). Both global and local hybrids destabilize surfaces and reduce adsorbate binding across the periodic table, in agreement with higher-level reference calculations. Density analysis reveals why hybrid functionals correct both quantities, whereas DFT+U does not. We recommend local, range-separated hybrids for the accurate modeling of catalysis in transition metal oxides at only a modest increase in computational cost over semi-local DFT.


2008 ◽  
Vol 128 (4) ◽  
pp. 044101 ◽  
Author(s):  
T. Gavin Williams ◽  
Nathan J. DeYonker ◽  
Angela K. Wilson

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