ELECTRONIC-STRUCTURE OF STRAINED SILICON-BRIDGED AND SULFUR-BRIDGED [1]FERROCENOPHANES AND AN ANALOGOUS DICARBON-BRIDGED [2]FERROCENOPHANE - AN INVESTIGATION BY PHOTOELECTRON-SPECTROSCOPY AND DENSITY-FUNCTIONAL THEORY
S. Barlow et al., ELECTRONIC-STRUCTURE OF STRAINED SILICON-BRIDGED AND SULFUR-BRIDGED [1]FERROCENOPHANES AND AN ANALOGOUS DICARBON-BRIDGED [2]FERROCENOPHANE - AN INVESTIGATION BY PHOTOELECTRON-SPECTROSCOPY AND DENSITY-FUNCTIONAL THEORY, Organometallics, 17(10), 1998, pp. 2113-2120
He I and He II photoelectron (PE) spectra of [Fe(eta-C5H4)(2)SiMe2] (1
), [Fe(eta-C5H3Me)(2)SiMe2] (2), [Fe(eta-C5H4)(eta-C5Me4)SiMe2] (3), [
Fe(eta-C5Me4)(2)SiMe2] (4), [Fe(eta-C5H4)(2)C2H4] (5), and [Fe(eta-C5H
4)(2)S] (6) have been measured and assigned. The d bands of 1-5 show l
ess structure than that of ferrocene, consistent with a loss of degene
racy of the e(2) orbitals on bending. Compound 6, which has the larges
t inter-ring angle of the series, shows two separate d bands. The tren
d in the first ionization energy closely parallels the variation in ox
idation potential. Density functional calculations on 1, 5, and 6 give
geometries in good agreement with the structures found from X-ray dif
fraction. Ionization energies calculated were also in excellent agreem
ent with experiment. Good agreement was also found between the calcula
ted d-d transitions and the position of the first spin-allowed band in
the optical spectra of 1 and 6. Estimates of strain energy in bending
ferrocene and octamethylferrocene were obtained, and octamethylferroc
ene was shown to be significantly more difficult to bend. Compounds 1
and 6 were both shown to have a low-lying empty orbital, partially loc
ated on the ipso carbon, which is a possible site for nucleophilic att
ack in the polymerization process undergone by these compounds.