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91.
92.
Summary For visual analysis of the density reorganization and distortion, the one-dimensional cut (x, y
0,z
0) and the two-dimensional cut (x, y, z
0) of the three-dimensional electron density difference function (x, y, z) are frequently employed. However, these cut functions do not satisfy any sum rules in contrast to the original difference function (x, y, z). To avoid this difficulty, the use of the marginal electron density functions
x
(x) and
xy
(x, y) and their difference functions
x
(x) and
xy
(x, y) is proposed. The marginal densities are condensation of the three-dimensional density onto a particular plane or line of our interest, and they satisfy the sum rule (i.e., the conservation of the number of electrons) exactly. Some basic properties of the marginal electron density are clarified for typical diatomic molecular orbitals. An illustrative application is given for the bonding and antibonding processes in the H2 system. 相似文献
93.
94.
Hans-René Bjørsvik José Angel Vedia Merinero Lucia Liguori 《Tetrahedron letters》2004,45(47):8615-8620
A new catalytic oxidation method for the preparation of aromatic carboxylic acids from methyl aryl ketones is reported. The method is an alternative to the haloform reaction; it is benign and affords the desired product without production of any harmful side products. The catalytic cycle is based on the use of an electron-deficient nitroarene as catalyst with either of the two cheap and green oxidants sodium percarbonate or sodium perborate. The method gives a good yield (87%) and shows excellent selectivity when the model substrate (acetophenone) is oxidized. A series of benzoic acids of industrial interest were prepared by means of this method. 相似文献
95.
A novel mixed valent tellurium oxide, SrTe3O8, has been synthesized and its crystal structure was determined ab initio from powder X-ray diffraction data. This oxide, which crystallizes in a tetragonal unit-cell, P42/m space group, with very close a and c cell parameters (6.8257(1) and 6.7603(1) Å, respectively), exhibits a very original structure built up of corner-sharing TeO6 (Te6+) octahedra and Te2O8 (Te4+) twin-pyramidal units. The latter ones form [Te3O8]∞ chains running along the [001] and the [110] directions. Besides the four sided tunnels where the Sr2+ cations are located, there are very large four sided tunnels running along the c-axis which are obstructed by the electronic lone pairs of the Te4+ cations. 相似文献
96.
Gerd Meyer 《无机化学与普通化学杂志》1992,618(12):18-25
CS[Er6C]I12 and cs2Lu[Lu6C]CI18: Examples for Quaternary Reduced Halides of the Lanthanides with Isolated “Clusters” Cs[Er6C]I12 and Cs2Lu[Lu6C]Cl18 were obtained as byproducts through metallothermic reductions of ErI3 and LuCl, with cesium in the presence of carbon in sealed tantalum containers at temperatures ranging from 700 to 940 °C. Cs2Lu[Lu6C]Cl18 (isostructural with Cs2Zr[Zr6H]Cl18, R 3 , a = 981.7 pm, c = 2723.2 pm, Z = 3, R = 0.082, R, = 0.053) contains octahedral [Lu6C] clusters which are slightly compressed along the threefold axis and edge-bridged by twelve chloride anions to form [Lu6C]Cl12 units. Six additional Cl in exo positions of the cluster provide octahedral coordination for the seventh Lu3+. Cs+ occupies anticuboctahedral interstices within the Cl+ layers as a part of the (hexagonal) closest packed arrangement. Cs[Er6C]I12 (trigonal, R 3, a = 1112.0pm, c = 2063.8pm, Z = 3, R = 0.094, R, = 0.068) exhibits [Er6C]I12 units as well and shows the structural framework of Sc[Sc6N]Cl12. Instead of Sc3+ in octahedral holes, cesium occupies a regular iodide position within the ccp sheets forming [CsI3] layers. Both halides are compared with other compounds of the lanthanides containing isolated [M6X12] clusters. The extreme electron deficiency is discussed. 相似文献
97.
Branko S. Jursic 《Theoretical chemistry accounts》1998,99(5):289-294
A computational study of perfluorinated methane derivatives was performed with complete basis set ab initio methods. The
total energies for their neutral, cation, and anionic states were computed. From these values, the energy gaps between different
electronic states, ionization potentials, electron affinities, and C-F bond dissociation energies were calculated. The computed
values are compared with experimental data and the reliability of complete basis set ab initio methods is discussed. New values
for C-F bond dissociation energies are suggested.
Received: 12 January 1998 / Accepted: 2 April 1998 / Published online: 29 July 1998 相似文献
98.
Todd B. Kreutzian Khalid S. A. Seraj Larry G. Anderson Donald C. Zapien 《Electroanalysis》2007,19(23):2479-2482
In this work, long optical path length thin‐layer electrochemical cell was constructed using indium‐tin oxide on glass as the electrode material. Iron release from ferritin adsorbed on the electrode was induced by applying a negative potential sweep in the presence of 1,10‐phenanthroline. The usefulness of spectroelectrochemistry as a means of determining the quantity of iron released from an adsorbed layer of ferritin is demonstrated. 相似文献
99.
The rate of electron transfer from organic sulfides to [CrV(ehba)2]− (ehba-2-ethyl-2-hydroxy butyric acid) decreases with a decrease in the polarity of the medium. The anionic surfactant, SDS and the cationic surfactant, CTAB have different effects on the kinetics of this reaction. The micellar inhibition observed in the presence of SDS is probably due to the decrease in the polarity and the electrostatic repulsion faced by the anionic oxidant from the anionic micelle and the partition of the hydrophobic substrate between the aqueous and micellar phases. The micellar catalysis in the presence of CTAB is attributed to the increase in the concentration of both reactants in the micellar phase. This micellar catalysis is observed to offset the retarding effects of the less polar micellar medium and the unfavorable charge-charge interaction between the + charge developed on S center in the transition state and the cationic micelle. This catalysis is contrary to the enormous micellar inhibition observed with IO4−, HSO5− and HCO4− oxidation of organic sulfides. 相似文献
100.
A polarizable molecular dynamics model for adiabatic electron transfer across the electrode|electrolyte interface is presented. The electronic polarizability of the water and of the metal electrode is accounted for by a dynamical fluctuating charge algorithm, image charges, and the Ewald summation adapted for a conducting interface. The effects of the solvent electronic polarizability are studied by computing the diabatic and adiabatic free energy curves for both polarizable and non-polarizable water models. This represents the first effort to compute the adiabatic free energy curves from simulation for a fully polarizable electrochemical system. 相似文献