184
A.S. Batsano6 et al. / Journal of Organometallic Chemistry 631 (2001) 181–187
,
der Waals radius of H (1.01 A) [17] and theoretically
The Cr···F interactions in 1 and 2 do not affect the
CꢀF bond lengths significantly. This is not surprising,
since the lone electron pairs of fluorine, which interact
with the vacant metal d-orbitals, are of essentially
p-character and hybridise little with the bonding
electrons.
,
calculated [18] radii of isolated atoms of Cr (2.42 A)
,
and Mo (2.56 A).
This effect could be explained in terms of the sheer
bulkiness of the aryl ligands, which push away the
imido ligands and ‘wedge’ the methyl groups into the
coordination sphere. However, the MꢀCꢀC angles of
each arene ligand are asymmetric, the smaller angle
being on the side of the M···H contact, implying attrac-
tive M···H interactions (adding to the 16-electron va-
lence shell of the metal atom) rather than forced
repulsive contacts. Simple steric repulsion energy calcu-
lations failed to reproduce the experimental molecular
geometry of 5 and 6 [15], which also supports the
existence of specific bonding interactions.
Molecules 1, 2 and 4 show even stronger distortions
of the same type. The CꢀMꢀC angles (138–140°) are
far wider than in 5 or 6 (121–123°), or in any transition
metal complex of this type, available in the Cambridge
Crystallographic Database (95–125°, average 111°)
[19]. The additional coordination sites are occupied by
two fluorine atoms from different fmes ligands, F(1)
and F(10) in 1 and 2. The M···F contacts are even
shorter than the M···H contacts in 5 and 6, even though
the van der Waals radius of F exceeds that of H by ca.
Further evidence of metal–fluorine interaction is pro-
vided by NMR spectra. Earlier we have found [7] that
both 1H and 19F spectra of complex 4 in solution
indicate a restricted rotation (‘locked’ conformation) of
ortho-CF3 groups of the fmes ligands below 323 K.
Although variable-temperature NMR experiments have
not been carried out in the present case, similar effects
were observed for complexes 1 and 2 even at room
temperature, indicating the existence of Cr···F interac-
tions in solution, probably of the same kind as were
found in the solid state. In contrast, the para-CF3
groups of fmes must have a very low rotation barrier.
Both such groups in molecule 1 are rotationally disor-
dered. For one of them the disorder was approximated
by two sets of fluorine atom positions with equal
occupancy (50%), for the other we could not find a
satisfactory model, while anisotropic refinement of only
one orientation left substantial diffuse residual electron
−3
,
density between the fluorine atoms (up to 0.7 e A
,
−3
,
,
0.3 A [17]. The Cr···F distances of 2.443(2) and 2.462(2)
A in 1, and 2.421(5) and 2.468(5) A in 2, are intermedi-
ate between the standard single bond in coordination
compounds of 1.870 A [20] and the sum of the van der
Waals radii of ca. 3.7 A [17,18]. Indeed they are com-
parable with the axial CrꢀF distance of 2.43 A in CrF2
[21], and cation–anion contacts of 2.449(5) A in
compared to 0.2 e A
elsewhere in the structure). In
,
,
structure 2, both para-CF3 groups also displayed very
large and elongated displacement ellipsoids of the
fluorine atoms, notwithstanding the low temperature at
which both structures were studied.
,
,
,
It is interesting to compare the coordination of the
Cr and Mo atoms in 1, 2 and 4. The molybdenum atom
is larger than chromium, as shown by the covalent radii
,
,
[Cr(py)4](PF6)2 [22] and 2.407(2) A in [Cr(NCMe)4]-
,
(BF4)2 [23]. It is noteworthy that the latter compound
has the cation and anion strongly associated even in
solution, as indicated by its low conductivity [23]. These
interactions can be regarded as hypervalent bonds (or,
in valence bond terms, as a covalent bondlion pair
resonance) [24]. The order 6 for the bond length d can
be roughly estimated by the formula 6=exp[(R−d)/
0.34], where R is the bond-valence parameter (for
of 1.27 and 1.10 A, respectively [27]. In agreement with
this, both the MꢀN and MꢀC bond lengths in 4 exceed
,
those in 1 and 2 by ca. 0.1 A. Sterically, there is nothing
to prevent the M···F distances elongating proportion-
ally to the covalent bonds, i.e. the whole coordination
sphere expanding isotropically. However, the Mo···F
,
distances are only 0.02 A longer than those for Cr···F,
suggesting relatively stronger attractive interactions
,
,
Cr(VI)ꢀF equal to 1.74 A) [25], yielding 6=0.12 for 1
with Mo (6=0.14, assuming R=1.81 A [25]). It is
noteworthy that Mo···H distances in 6 are shorter than
and 2. The metal coordination in complexes 1 and 2
can thus be described as 4+2, or intermediate between
tetrahedral and octahedral, including secondary MꢀF
bonding. The coordination chemistry of the CF unit in
fluorocarbons towards metal centres has been exten-
sively reviewed by Plenio [12]. In the first transition
series, however, there were considered to be only two
convincing reports of such interaction, one being a very
,
Cr···H in 5, by an average of 0.17 A.
MꢀC distances in complexes 1, 2 and 4 are longer
than in 5 and 6 by ca. 0.1 A. These s-bonds are
,
augmented by dp(M)pp(C) back-bonding, which
weakens as the CꢀMꢀC angle increases, since the two
ligands are increasingly competing for the same (occu-
pied) metal d-orbital. All imido-ligands in the com-
plexes under consideration can be described as ‘linear’,
although, as indicated earlier, there is competition be-
tween p-donor ligands in a tetrahedral environment,
since only three of the possible four p-bonds can be
formed between the metal and the cis-imido ligands.
Their MꢀNꢀC angles vary considerably without a cor-
,
short F···Ti distance of 2.151(2) A in [Cp*Ti(FPh)]-
[BPh4] [26] and the other in the complex [VCl(fmes)2-
(thf)], discussed above [6]. More examples were de-
scribed for metals in the second transition metal series
[12], but none for molybdenum, apart from compound
4 [7] (see above).
2