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and 6-membered fused metallacycles and bite angles (P11-Ni-
P12) that are much greater than in their POCOP analogues fea-
turing two fused 5-membered metallacycles (ca. 170–1768 vs.
1648).[21] The bite angles in [(RPIMCOPR’)NiBr] are also influenced
by the P-substituents, being roughly 6–78 wider in the struc-
tures of 3b and 3c bearing the bulkier iPr2P moieties. Steric
factors appear to have less influence over bond lengths, but
the NiÀP distances in 3a and 3b (R=R’: 2.132–2.134 and
2.168–2.169 ) are significantly shorter than those in 3c (R¼ R’:
2.138 and 2.199 ).
A distorted square-planar geometry is also adopted by the
[(NHCCOPR’)NiBr] complexes 5a and b, and minimal structural
variations result from the different P-substituents. The small
bite angles (ca. 161–1628) can be attributed to the metallacycle
size (5,5) and correlated with the shorter N1ÀC7 bonds in 5a
and 5b relative to the OÀP bonds in the analogous POCOP
complexes.[22] The NiÀP1 distances in 5a and 5b (av. 2.147 )
are longer than those in 3a and 3c (av. 2.133 ) but remain
comparable to the corresponding distance in a typical POCOP
structure (2.148 ).[13,22] These observations establish the fol-
lowing order of trans influence: ArOP(iPr)2 ꢁNHC>2-imidazol-
yl-PPh2. The NiÀCN2 distances of approximately 1.95 in 5a
and 5b are longer than the corresponding distances of ap-
proximately 1.90–1.92 found in previously reported Ni–NHC
complexes.[23] Finally, the central NiÀC1 bond lengths are much
shorter in the 5,5-complexes 5a and 5b than in the 5,6-com-
plexes 3a–c (1.87 vs. 1.94 ).
Figure 3. Molecular views of 6b (top) and 8a (bottom). Thermal ellipsoids
are drawn at the 50% probability level and the H atoms and the triflate
anion have been omitted for clarity. Selected bond lengths () and bond
angles (8) for 6b: NiÀC1 1.944(2), NiÀN 1.882(2), NiÀP1 2.1572(5), NiÀP2
2.2005(5); P1-Ni-P2 175.70(2), C1-Ni-N 168.92(7), Ni-N-C 172.48(15). Selected
bond lengths () and bond angles (8) for 8a: NiÀC1 1.876(4), NiÀN 1.888(4),
NiÀP1 2.166(2), NiÀC7 1.943(5); P1-Ni-C7 161.0(2), C1-Ni-N 177.5(2), Ni-N-C
177.3(4).
The crystal structures of the cationic complexes 6b and 8a
(Figure 3) also revealed a somewhat distorted square-planar
geometry around the Ni center. The above-noted smaller bite
angle P1-Ni-C7 and shorter NiÀC1 bond in NHCCOP complexes
are confirmed here. Likewise, the NiÀP1 bond lengths in 6b
(ca. 2.157 ) and 8a (ca. 2.166 ) reflect the superior trans in-
fluence of the NHC moiety, even though the PR2 moieties
being compared are different. A greater deviation from the
ideally linear NiÀNCMe coordination mode is found in 6b than
in 8a: C1-Ni-Nꢁ1698 vs. 1788; Ni-N-Cꢁ1728 vs. 1778. This de-
viation is likely caused by the steric demand of the inserted
iPr2P moiety in 6b.
features, whereas the extent of d deshielding upon N-meth-
31P
ylation depends on the P-substituents (by ca. 8 ppm for 3a!
4a vs. 21 ppm for 3b!4b). The N+ÀCH3 substituent of the
1
[(PIMIOCOP)NiX] complexes gives a single H NMR resonance
at dH ꢁ +3.2 ppm. Finally, the NHCCOP complexes 5a,b and
8a,b display characteristic 13C NMR carbene signals at dC
ꢁ172–175 ppm [d; 2J(C,P)ꢁ90–110 Hz].
IR spectroscopy, cyclic voltammetry, and theoretical studies
In an effort to estimate the electronic density of the Ni center
in the title complexes, the oxidation potentials Eopx and IR CꢀN
stretching frequencies n(CꢀN) were measured. Wide-scope
computational studies at the density functional theory (DFT)
level were also performed on the cationic acetonitrile adducts
6a,b, 7a,b, 8a,b, and their previously reported POCOP ana-
logues 9a,b (Figure 4).[13,22] The results that are most pertinent
to the present discussion are presented sequentially in the fol-
lowing sections and some of the computational results (includ-
ing geometry optimization studies, Figures S3–S10 and Ta-
bles S3–S8) are provided in the Supporting Information.
Characterization of the proligands and complexes by NMR
spectroscopy
R
The most characteristic NMR features of the PIMCOPR’ proli-
gands 2b and 2c consist of the pair of singlet 31P resonances
for the phosphinite and imidazolophosphine moieties, as well
as the 13C signals for the central C nuclei that are flanked by
3
4
these moieties [dC ꢁ118–119 ppm (dd); J(C,P)ꢁ7–8 Hz, J(C,P’)
ꢁ3–5 Hz].[12] Upon nickelation, a dramatic 31P downfield shift
occurs, giving rise to doublets of doublets with 2J(P,P’)>
300 Hz, as anticipated for the two inequivalent and mutually
trans P nuclei.[24] The 13C resonances for the reacting carbon
nucleus also moved downfield and turned into pseudo-triplets
Measured and calculated n(CꢀN): IR stretching frequencies
n(CꢀN) of coordinated acetonitrile molecules are a priori ex-
pected to reflect the overall donor character (s-donating vs. p-
accepting properties) of coligands. It was indeed reported that
the (a priori nonbonding) lone pair of a nitrile, which is strong-
ly polarized on the nitrogen lone pair, could actually exhibit
some antibonding character. Therefore, n(CꢀN) values are ex-
pected to increase upon s-donation from the coordinated ace-
2
2
[dC ꢁ125 ppm; J(C,P)ꢁ J(C,P’)ꢁ22 Hz].
Conversion of the PIMCOP complexes 3a,b and PIMIOCOP
complexes 4a,b into their respective cationic acetonitrile ad-
ducts 6a,b and 7a,b has a relatively minor impact on the NMR
Chem. Eur. J. 2015, 21, 17403 – 17414
17406
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