Synthesis and structural studies of bis(1,10-phenanthrolinethiocyanatemercury) tetracarbonyliron

The bis(1,10-phenanthrolinethiocyanatemercury)tetracarbonyliron was prepared from bis(thiocyanatemercury)tetracarbonyliron and 1,10-phenanthroline and crystallized from hot acetone solution as [Fe(CO)4(HgSCN)2(phen)2]·C3H6O, which was subjected to a full IR and X-ray crystallographic characterization. The iron atom is octahedrally coordinated by four carbonyl groups and two mercury atoms in cis positions. The coordination geometry of the mercury atoms is a distorted square-based pyramid since each one is coordinated to one iron, one sulphur, one mercury and two nitrogen atoms. The FeHg distances are 2.549(3) and 2.564(3) Å, and the HgFeHg angle is 78.01(9)°. © 1992.

Synthesis and structural studies of (3,5-dinitrobenzoate)bis(triphenylphosphine)copper(I)

The compound (3,5-dinitrobenzoate)bis(triphenylphosphine)copper(I) was synthesized and studied by IR spectroscopy and X-ray diffraction techniques. It is monomeric with the carboxylato acting as a monodentate ligand. The copper atom shows a trigonal planar coordination geometry. © 1993.

Synthesis, characterization and molecular structures of the pyridinium trans-bis(pyridine)tetrachlororuthenate(III) and pyridinium trans-(carbonyl)(pyridine)tetrachlororuthenate(III)

The pyH[trans-RuCl4(py)2](1) and pyH[trans-RuCl4(CO)(py)](2) complexes were synthesized and found to crystallize in space group P21/n, Z = 4 with a = 8.080(7), b = 22.503(7), c = 10.125(6) Å, β = 93.19(6)° for (1) and a = 7.821(1), b = 10.337(3), c = 19.763(3) Å, β = 93.07(1)° for (2). The structures were solved by Patterson and difference Fourier techniques and refined to R = 0.062 for (1) and R = 0.038 for (2). In both cases the Ru(III) ion is octahedrally coordinated to four co-planar chlorine atoms, the nitrogen of the pyridine rings or carbon from the carbon monoxide. Another protonated pyridine group, which forms the counter-cation completes the crystal structures. The UV-Vis absorption spectra show three bands: (1) 360 (ε = 1180 M-1 cm-1), 441 (ε = 3200 M-1 cm-1) and 532 nm (ε = 400 M-1 cm-1); (2) 315(ε = 1150 M-1 cm-1), 442 (ε = 3170 M-1 cm-1) and 530 nm (ε = 390 M-1 cm-1). The two higher energy bands were associated with ligand-to-metal charge transfer transitions and a third band at lower energy was assigned to a d-d transition. Low temperature EPR data confirmed the presence of the paramagnetically active Ru(III) and it is consistent with axial symmetry of the complexes. The position of the stretching CO band in complex (2) is discussed in terms of metal-CO backbonding.

A description of ligand field effects in the Di-μ-Azido-Bis [{Azido(N,N-diethylethylenediamine)}Copper(II)] compound by the simple overlap model

We present a theoretical description of ligand field effects in the di-μ-azido- bis[{azido(N,N-diethylethylenediamine)} copper(II)] compound by the Simple Overlap Model. The ligand field Hamiltonian is expressed in terms of irreducible tensor operators for an assumed D3h site symmetry occupied by the copper ion. The ligand field parameters, calculated from the available structural data, indicate that the copper ion is under the influence of a very strong ligand field. The energy of the d-d absorption band is well reproduced phenomenologically by the model.