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Phosphine vibrational frequency

Studies on the solid-state structures, vibrational frequencies and dipole moments of tertiary phosphine chalcogenides have shown the phosphorus to be in an approximately tetrahedral environment with phosphorus-chalcogen bond lengths in-between those expected for single and double bonds.21 There has been much debate on the nature of the phosphorus-chalcogen bond in these... [Pg.291]

The various physical techniques that we might use to study molecular species depend on a variety of proeesses. The conclusions we could draw about structures are related to the timescales associated with these proeesses, and it is important for us to understand these if we are to avoid making erroneous deductions. In relation to any one type of experiment, there are in fact four different times for us to consider the time during which a quantum of radiation or a particle can interact with a molecule the lifetime of any excited state of the molecule the minimum lifetime that the species being studied must have to allow it to be seen as a distinct species and the total duration of an experiment in which the species is observed, which may be as much as several hours or as little as 10 s. Before we consider these further, we must look at the timescales of typical molecular processes so that we can relate them to timescales associated with structural techniques. Typical vibrational frequencies are of the order of lO to 10 Hz, while rotational frequencies are around 10 ° to 10 Hz. The inversion of ammonia has a rate of about 10 Hz at room temperature, while the corresponding rate for phosphine is 10 Hz. The inversion rate for methane is 10 Hz, so any one molecule inverts, on average, once every 100 million years But remember that there are 6 x 10 molecules in a mole of gas, so in fact the inversion is by no means a rare occurrence. Pseudorotation in PF5, which switches axial and equatorial fluorine atoms, has a rate of about 10 Hz at room temperature, while the rate for PCI5 is 10 Hz. [Pg.24]

Here, the author considers that the introduction of low-vibrational frequency (LVF) ligands as a linker part in the polymer chains would result in the preparation of a lanthanide coordination polymer with strong luminescence properties. Strongly liuninescent lanthanide complexes composed of LVF hfa and bidentate phosphine oxide ligands have been described in former chapters. The author also proposes that the introduction of aromatic aryl groups in the linker part of lanthanide coordination polymer is effective for the construction of thermostable luminophores with intermolecular interactions, such as CH/F, n-n, and CWn interactions. [Pg.15]

The electronic contribution by a phosphine was originally measured by IR spectroscopy. The vibrational frequencies of [Ni(CO)3(PR3)] for a number of complexes differing in R were measured. The stretching frequency of the carbonyl is inversely related to the extent of back donation. Since both CO and PRj compete for back donation from the metal, the stretching frequency of the carbonyl is an approximate measure of the donor-acceptor properties of PRj. [Pg.35]

Two other publications on Ir (73 keV) Mossbauer spectroscopy of complex compounds of iridium have been reported by Williams et al. [291,292]. In their first article [291], they have shown that the additive model suggested by Bancroft [293] does not account satisfactorily for the partial isomer shift and partial quadrupole splitting in Ir(lll) complexes. Their second article [292] deals with four-coordinate formally lr(l) complexes. They observed, like other authors on similar low-valent iridium compounds [284], only small differences in the isomer shifts, which they attributed to the interaction between the metal-ligand bonds leading to compensation effects. Their interpretation is supported by changes in the NMR data of the phosphine ligands and in the frequency of the carbonyl stretching vibration. [Pg.328]

Assignments. - Electric modulation of vibrational rotational bands of polar molecules included a study of phosphine.120 Ringbending (puckering) transition frequencies have been measured for the phospholene (42) for the ground and excited states.121 The PD deformation band for the sulphide (43) has been assigned.122... [Pg.405]

DFT calculations were performed on Mo dinitrogen, hydra-zido(2-) and hydrazidium complexes. The calculations are based on available X-ray crystal structures, simplifying the phosphine ligands by PH3 groups. Vibrational spectroscopic data were then evaluated with a quantum chemistry-assisted normal coordinate analysis (QCA-NCA) which involves calculation of the / matrix by DFT and subsequent fitting of important force constants to match selected experimentally observed frequencies, in particular v(NN), v(MN), and 8(MNN) (M = Mo, W). Furthermore time-dependent (TD-) DFT was employed to calculate electronic transitions, which were then compared to experimental UVATs absorption spectra (16). As a result, a close check of the quality of the quantum chemical calculations was obtained. This allowed us to employ these calculations as well as to understand the chemical reactivity of the intermediates of N2 fixation (cf. Section III). [Pg.372]


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See also in sourсe #XX -- [ Pg.236 ]




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