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reaction of (Cy2N)3TiCl with n-butyllithium in n-hexane at
−30 °C produces the butylated complex (Cy2N)3TinBu (3a) in
moderate yield. Single crystals of 3a suitable for X-ray
diffraction analysis could be obtained from a saturated n-
hexane solution at 0 °C.
Complex 3a crystallizes in the triclinic space group P1. The
̅
ORTEP plot is given in Figure 4. Analogous to the zirconium
Figure 3. Molecular structure of complex 3b. Thermal ellipsoids are
drawn at the 50% probability level. Hydrogen atoms are omitted for
clarity. Selected bond lengths [Å] and angles [deg]: Zr1−N1
2.0651(8), Zr1−N2 2.0612(8), Zr1−N3 2.0616(8), Zr1−C37
2.2938(10), N1−C1 1.4790(12), N1−C7 1.4709(12), N2−C13
1.4791(12), N2−C19 1.4684(12), N3−C25 1.4784(12), N1−C31
1.4683(12), N1−Zr1−N2 112.10(3), N1−Zr1−N3 113.63(3), N1−
Zr1−C37 105.55(3), N2−Zr1−N3 111.48(3), Zr1−N1−C1
108.27(5), Zr1−N1−C7 136.59(6), C7−N1−C1 114.95(7), Zr1−
N2−C13 104.88(5), Zr1−N2−C19 137.91(6), C13−N2−C19
117.13(7), Zr1−N3−C25 106.72(5), Zr1−N3−C31 136.98(6),
C25−N3−C31 116.23(7).
Figure 4. Molecular structure of complex 3a. Thermal ellipsoids are
drawn at the 50% probability level. Hydrogen atoms and the second
position of the disordered part of the molecule are omitted for clarity.
Selected bond lengths [Å] and angles [deg]: Ti1−N1 1.9150(10),
Ti1−N2 1.9184(10), Ti1−N3 1.9101(8), Ti1−C37 2.1464(10), N1−
C1 1.4795(3), N1−C7A 1.503(2), N2−C13 1.4759(13), N2−C19A
1.5162(19), N3−C25 1.4803(12), N1−C31 1.4693(12), N1−Ti1−N2
111.27(4), N1−Ti1−N3 109.58(4), N1−Ti1−C37 111.16(4), N2−
Ti1−N3 113.22(4), Ti1−N1−C1 113.58(6), Ti1−N1−C7A
117.79(11), C7A−N1−C1 128.63(12), Ti1−N2−C13 108.85(6),
Ti1−N2−C19A 139.95(10), C13−N2−C19A 111.18(11), Ti1−N3−
C25 114.37(6), Ti1−N3−C31 124.48(6), C25−N3−C31 121.14(7).
corresponding titanium complexes (Cy2N)3TiCl (1a) and
(Cy2N)3TiMe (2a) as well.24 Another interesting feature of
the solid-state structures is a short intramolecular contact
between the metal center and one ipso carbon of each
dicyclohexylamine ligand (see Supporting Information, Table
S5). They are significantly shorter (on average 0.85 Å) than the
sum of the van der Waals radii of zirconium and carbon. These
close contacts are typical for complexes with this bulky
secondary amine ligand.24,25 Similar to the methylated complex
2b, temperature-dependent 1H NMR spectroscopic experi-
ments demonstrate that the monobutyl complex 3b is rather
stable. First indications for a degradation process can be noticed
at 80 °C. After 16 h at 100 °C the characteristic signal of the
ipso protons has completely disappeared, but cyclohexene is
released. The remaining decomposition products could not be
identified yet. Especially dialkyl complexes of zirconium are
known for β-H elimination reactions at low temperatures. The
Negishi system Cp2ZrCl2/n-butyllithium has to be prepared at
−78 °C and eliminates 1-butene and butane to yield a
zirconocene intermediate, which can undergo various reac-
tions.42−45 To our knowledge there are only two comparable
monobutylated complexes, reported by Jia, Brennessel, et al.11
These compounds exhibit an n-butyl group and three nitrogen-
containing ligands like complex 3b. Solid-state structures reveal
indications for weak β-agostic interactions. The Zr−Cα−Cβ
angle of 95.7° and 97.1°, respectively, is much smaller than the
corresponding angle in nonagostic compounds (108−126°),
but larger than angles in known β-agostic complexes (about
85°).46−48 The Zr−Cα−Cβ angle in complex 3b is 125.26(7)°.
We assume that the electron deficiency of the metal center is
compensated due to the good N(pπ)−Zr(dπ) interactions
between the secondary amine ligands and the metal.
Furthermore, the solid structure of 3b indicates that there is
no space for an interaction between the metal center and the
butyl group because of the high steric hindrance achieved by
the bulky cyclohexyl groups.
compound (3b) the central titanium atom is slightly distorted
tetrahedral coordinated. The titanium−nitrogen distances are
of comparable length (Ti1−N1 1.9150(10) Å, Ti1−N2
1.9184(10) Å, Ti1−N3 1.9101(8) Å). The Ti−N bonds and
the Ti1−C37 bond length of 2.1464(10) Å are within the range
for comparable complexes.5,24 All nitrogen atoms are trigonal
planar coordinated (sum of all angles: N1: 360°, N2: 360°, N3:
360°).The solid-state structure gives no evidence for a β-agostic
interaction. The angle Ti1−C37−C38 is 123.34(7)°, which is a
typical value for known nonagostic compounds.46−48 As
explained earlier for the corresponding zirconium complex,
we suspect that the sterical hindrance of the amido ligands and
the reduced Lewis acidity because of the N(pπ)−Ti(dπ)
interactions are responsible for this effect.
However, the titanium compound 3a is considerably less
1
stable compared to the analogous zirconium complex 3b. H
NMR spectroscopic experiments show a complete degradation
in solution at ambient temperature within 1 day, while
cyclohexene is released. Furthermore, the formation of the
binuclear imido-bridged titanium complex could be found after
a certain time. This indicates a similar degradation process for
the methylated (2a) and the butylated complexes (3a)
(Scheme 2).24 There are no hints for a butyl-specific β-C−H
elimination reaction at the alkyl chain.
In summary, we demonstrated the preparation of mono-
alkylated dicyclohexylamido titanium and zirconium complexes
from the corresponding chlorines by the use of methyl- and
butyllithium, respectively. The molecular structures of the
chlorine 1b and the alkylated complexes 2b, 3a, and 3b could
Due to the unexpected stability of complex 3b, we
transferred the synthetic procedure to titanium. The equimolar
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dx.doi.org/10.1021/om5008105 | Organometallics 2014, 33, 7011−7014