Chemistry Reference
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Tab. 1.2 (C=C)
vertical ionization potentials of conjugated ylides IE 2 or IE 1 and related
-
hydrocarbons (IE 1 ).
IE 2 or IE 1 (Ylide) a)
[eV]
IE 1 ( -Hydrocarbon) [eV]
Me 3 P=CH- CH=CH 2
9.02 (IE 2 )
Ethylene: 10.51
Me 3 P= C 5 H 4
6.82 (IE 1 ) !
Butadiene: 9.10
Me 3 P=CH- C 6 H 5
8.32 (IE 2 )
Benzene: 9.25
a) Ionization from (C=C)
localized orbitals.
species with ylide ligands sometimes in bridging or in chelating function. In
Fig. 1.1, A represents the fundamental monodentate
-complex. Its metal-carbon
bond can be described simply as the result of a two electron/two orbital stabilizing
interaction between the high lying carbon-centered ylide HOMO “n C - ” and a vacant
metal orbital. For a given ylide, the degree of complex stabilization depends on the
energy of the interacting metal orbital(s), which can be tuned chemically with the
other ligands attached to the metal. In B and C hydrocarbon
-systems are attached
to the ylidic carbon which not only results in a delocalization of electron density but
also raises the energy levels of the
-substituents with respect to the unperturbed
parent
-hydrocarbon, i.e., for the ligands in B and C relative to ethylene and cis- bu-
tadiene (Tab. 1.2). In the exceptional case of cyclopentadienylidenephosphoranes
(R 3 PC 5 H 4 ) the extreme perturbation of the
-substituent pushes the corresponding
cis -butadiene level even slightly above that of the ylide bond n C - -level.
The enhanced energetic availability of the substituent
-electrons makes it clear
why strongly conjugated ylides may act as polyhapto
-ligands when metal local-
ized orbitals of appropriate symmetry are accessible. In extreme cases the location
of highest reactivity may shift into a position remote from the onium center. This
“activation” of a substituent, attached to the ylidic carbon, is a general feature and
is not limited to CC-
-systems. An impressive example is the photoelectron spec-
trum of acetylmethylene-trimethylphosphorane, where the low second ionization
potential IE 2 =8.2 eV originates essentially from an oxygen lone pair orbital [Eqs.
4
* K.A. Ostoja Starzewski, H. Blau, W. Malisch,
unpublished results
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