STRUCTURE AND BONDING OF SOLVATED MERCURY(II) AND THALLIUM(III) DIHALIDE AND DICYANIDE COMPLEXES BY XAFS SPECTROSCOPIC MEASUREMENTS AND THEORETICAL CALCULATIONS
R. Akesson et al., STRUCTURE AND BONDING OF SOLVATED MERCURY(II) AND THALLIUM(III) DIHALIDE AND DICYANIDE COMPLEXES BY XAFS SPECTROSCOPIC MEASUREMENTS AND THEORETICAL CALCULATIONS, Inorganic chemistry, 33(17), 1994, pp. 3715-3723
The solvation of mercury(II) complexes and ions has been studied by XA
FS methods and compared to the corresponding thallium(III) species. An
alyses of Hg L(III) edge extended X-ray absorption fine structure (EXA
FS) spectra gave the distances 2.29(2) and 2.31(2) angstrom for HgCl2
in aqueous and dimethyl sulfoxide solutions, respectively, 2.46(2) ang
strom for solid HgBr2 and 2.42(2) angstrom for HgBr2 in aqueous soluti
on; for Hg(CN)2 in aqueous solution Hg-C = 2.04(2) angstrom and Hg-N =
3.18 (3) angstrom. The weakness of the EXAFS signals observed of the
solvated Hg2+ ion in e.g. pyridine, acetonitrile, and aqueous solution
s are interpreted as being due to dynamic distortions of the first sol
vation shell by second-order Jahn-Teller effects. The pre-edge transit
ions in the X-ray absorption near-edge structure (XANES) region for me
rcury(II) and thallium(III) complexes have been used to distinguish be
tween different coordination geometries of the solvated species. Theor
etical ab initio calculations have been performed on the structures of
the mercury(II) and thallium(III) dihalide and dicyanide complexes, i
n order to compare the effects of differences in bonding and hydration
, and also on the valence shell energy levels, to assist assignments o
f pre-edge features in the XANES spectra. Relativistic effective core
potentials (ECP) were constructed, both for the ground-state mercury a
nd thallium atoms and for the 2p ionized state, and used in calculatio
ns at the MCPF level of bond lengths and relative energy differences.
The first pre-edge peak found for all complexes in their XANES spectra
was assigned to a (2p) --> SIGMA(g)+ (approximately Hg 6s) excitation
, with the splitting of the pre-peak for Hg(CN)2 possibly due to (2p)
--> PI(C-N) at ca. 3.4 eV higher energy. Multiple scattering resonanc
es have been discussed for the CN ligands. Comparisons of calculated a
nd experimental bond lengths of the mercury(II) and thallium(III) dich
loride and dicyanide complexes revealed unexpectedly short bond length
s for the mercury(II) complexes, which have been discussed in terms of
weaker solvation and stronger bonding. The bonding in the Hg(CN)2 and
Tl(CN)2+ complexes were analyzed by theoretical calculations using a
constrained space orbital variation (CSOV) technique, showing signific
ant contributions of back-donation particularly in the Hg-CN bonds. Th
e trends of the force constants from vibrational spectra are consisten
t with this picture and show stronger and shorter M-C bonds but also s
tronger C-N bonds in the Hg(CN)2 complex than in the Tl(CN)2+ complex.