V. H. Gessner and P. Schrçter
sulfonyl unit was also confirmed by the lower charge con-
centration at the methanide carbon (qC =À1.51) compared
with the bis(thiophosphinoyl) system (qC =À1.77)[11b] and by
the viability of the dilithiation, which is reflected by a re-
markably low reaction barrier of only 26.2 kJmolÀ1.
Concerning the planarization of the carbon atom, the or-
bital properties are of particular interest. The HOMO and
HOMO-1 of A (Figure 3c) represent the two lone pairs at
the methandiide carbon atom. The HOMO is essentially
nonbonding, whereas the HOMO-1 points towards one of
the lithium atoms. Natural bond orbital (NBO) analyses sug-
gests an approximately sp2 hybridized methanide carbon
with two nonequivalent lone pairs differing in their energy
and hybridization (LP(1)/HOMO-1: sp2-hybrid orbital
(sp1.99); LP(2)/HOMO: p-orbital (sp99.9)].[20,21] This orbital
representation is close to that of the planar bis(phosphoni-
um) system I. The energy-optimized structure of I also ex-
hibits two different NBOs for the lone pairs, however, with
a slightly higher p-character for LP(1) and thus a higher s-
Figure 4. Bonding modes of two lithium atoms with a sp2-hybridized
carbon atom and NBOs of LP(1) and LP(2) in a) planar arrangement
(Aꢀ) and b) distorted arrangement (B).
character in the C P bonds (sp1.45, sp2.10 for A). This is in
À
line with the observed broadened P-C-P angle (132.18) com-
pared with the P-C-S angle (121.48) in 1-Li2. To evaluate if
a higher p-character of the two lone pairs may also favor
a planar arrangement in 1-Li2, variations of model system A
were calculated: Aꢀ with a constrained planar Li-P-C-S-Li
moiety and A-131 and A-135 with P-C-S bond angles fixed
at 131 and 1358, respectively. Energy optimization revealed
À
À
(e.g., Wiberg bond indices for Li O and Li C: nWiberg <0.1),
which means that structure formation is dominated by the
interaction of charges and less by the overlap of orbitals.
This suggests that the isolation of further methandiides with
a planar four-coordinate carbon should be possible by care-
ful selection of the coordinating side arms and the reaction
conditions (additives). It will be interesting to see, if these
new bonding modes of carbon are maintained in complexes
with transition metals with carbon–metal bonds of more co-
valent character, and if this influences the reactivity of these
compounds.
an energetic preference of the model system
A by
21.6 kJmolÀ1 over its planar analogue and most importantly
a preference of a nonplanar arrangement in A-131 and A-
135. Interestingly, NBO analyses of these derivatives, includ-
ing the planar system Aꢀ, showed no significant changes in
the orbital interactions, so that in general all structures can
be described by a sp2-hybridized methanide carbon atom.
However, this orbital setting has been used to explain the
planar geometry at the methanide carbon in compound I.
Next question is: how is this then in line with the structure
of 1-Li2, especially given the nonplanar coordination and the
strongly distorted arrangement around C13 (Figure 2c).
Overall, the calculations indicate two borderline cases for
the bonding in methandiides shown in Figure 4: a) The four
substituents are exclusively bound to the sp2-hybrid orbitals
In conclusion, the synthesis and characterization of mono-
and dilithiated sulfonyl-substituted phosphine sulfide 1 was
presented. Upon metalation, dramatic changes in bond
lengths and angles of the methanide carbon were observed,
which resulted from rehybridization and electrostatic inter-
actions in the P-C-S backbone. The dilithio methandiide fea-
tures a distorted carbon environment, which crucially differs
from the tetrahedral arrangement. This geometry is caused
mainly by geometrical restriction of the donor functions and
can be described by two different bonding modes of the lith-
ium atoms with the sp2 hybridized carbon atom.
À
through two 2e,2c bonds (C X bonds) and one 2e,3c bond
(Li-C-Li) giving way to a planar four-coordinate carbon
atom (compound I). b) All substituents form 2e,2c bonds,
whereas one of the lithium atoms is bound to the p-orbital
at the carbon. This results in a strongly distorted tetrahedral
arrangement with a small Li-C-Li angle (Li3-C13B-Li4
97.8(2)8 in 1-Li2). Although the planar system I is described
by bonding mode a), for the description of the structure of
1-Li2 both bonding modes have to be applied. This can
easily be seen from the environments of C13 and C13B in
Figure 2 and was confirmed by NBO analysis of model
system B for the environment around C13 (Figure 4b and
the Supporting Information).
Acknowledgements
We thank the Deutsche Forschungsgemeinschaft, the Alexander von
Humboldt Foundation and the Fonds der Chemischen Industrie for finan-
cial support. We also thank Prof. Dr. H. Braunschweig for generous sup-
port and helpful advices.
One always has to keep in mind that the interactions in
dilithio methandiides are essentially electrostatic in nature
Keywords: alkali metals · carbanions · lithium · planar four-
coordinate carbon · structure elucidation
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ꢃ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 0000, 00, 0 – 0
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