Triad of Bis(orthometalated) d8-Complexes
Organometallics, Vol. 27, No. 20, 2008 5365
dppe and to uncoordinated PPh2 groups, respectively. The dppe
resonance of the nickel complex 6 is a well-resolved triplet with
a separation of 11.6 Hz, that of the palladium complex 7 is a
poorly resolved triplet (separation ca. 14 Hz), while that of 8 is
a broad singlet accompanied by 195Pt satellites (JPtP 2137 Hz).
The PPh2 resonances of 6-8 display an unexpected pattern,
consisting of a well-resolved doublet of doublets with separa-
tions of 26.8, 95.5 Hz (6), 25.9, 76.9 Hz (7), and 26.5, 81.5 Hz
(8). In the case of 8 there are also 195Pt satellites (JPtP 227 Hz),
somewhat greater than the corresponding values in [Pt(κC-2-
C6H4PPh2)2(dppe)] (170 Hz).32 The separations in the doublet
of doublets are not reproduced in the dppe resonance; hence
the unexpected pattern is not due to coupling with the 31P nuclei
of dppe. Likewise, the separations observed in the dppe
resonances of 6 and 7 are not reproduced in the corresponding
PPh2 resonances; hence these separations do not arise from
coupling with the 31P nuclei of the PPh2 groups. These
conclusions are supported by the failure to observe cross-peaks
in the 2D COSY 31P/31P NMR spectra. The uncoordinated PPh2
resonances of 9 and 10, in contrast with those of 6-8, are in
each case the expected singlet at ca. δ -6, with multiplet fine
structure, presumably due to 19F coupling.
due to F6 is shifted to higher frequency (δF ca. -105 in 6-8,
ca. -117 in 9 and 10) and in the case of 6-8 appears as a
doublet of multiplets. In the platinum(II) complex 8, the coupling
constant of 195Pt to F6 (326 Hz) is approximately double that
in the precursor 1 and is similar to the values reported for
coupling to the ortho-fluorine atoms in cis-[Pt(C6F5)2(PPh3)2]27
and [Pt(C6F5)2(dppe)]28 (see above). A 31P/19F heteronuclear
multiple quantum correlation (HMQC) experiment on the
palladium complex 7 showed well-defined cross-peaks associ-
ated with the resonances at δF -105.2 (F6) and -123.8 (F3);
the coupling constants are ca. 75 and 25 Hz, respectively, in
reasonable agreement with the separations observed in the 1D
31P NMR spectrum. A similar experiment on the nickel(II)-
bipy complex 9 also showed cross-peaks for the resonances at
δF -117.8 (F6) and -124.6 (F3), but the coupling to F6 (ca. 30
Hz) is clearly less than that in the dppe complex; the coupling
to F3 is less than 20 Hz. In the 1D 19F NMR spectrum of the
nickel-dppe complex 6, the doublet of multiplets due to F6 is
so well resolved that the coupling with phosphorus can be read
off directly; its value (98 Hz) is in fair agreement with the
separation of 95 Hz obtained from the 31P NMR spectrum. It
seems clear, therefore, that the separations of 75-95 and 25
Hz in the doublet of doublets pattern of the PPh2 resonances of
We thought at first that the doublet of doublets for the PPh2
groups in 6-8 might arise from inequivalence of the PPh2
groups in solution caused by restricted rotation about the
M-C6F4PPh2 bonds, even though this would have implied a
remarkably large, six-bond P-P coupling constant (ca. 26 Hz).
This explanation did not seem implausible given the ample
evidence for restricted rotation about M-C6F5 bonds40-49 and
for slowed rotation about M-P and P-C bonds in platinum(II)
complexes of (C6F5)3P.50-52 However, the frequency separation
between the pairs of doublets was found to be the same at 202.3
MHz as at 121.4 MHz; hence there is only one 31P chemical
shift and the observed pattern can only be due to P-F coupling.
4
3
6-8 are due to J and J P-F couplings, respectively.
In free pentafluorophenylphosphines, such as (C6F5)3P and
C6F5PPh2, the largest P-F coupling constant of ca. 38 Hz
(observed in the 19F NMR spectrum) is due to F2,6 (the ortho-
fluorines), the meta- and para-couplings being close to zero.29,53
Couplings similar to those of 6-8 are not observed in the 31P
NMR spectra of 2-BrC6F4PPh2 or 2-Me3SnC6F4PPh2.54 Possible
reasons for these differences will be discussed below.
Dinuclear and Tetranuclear Complexes of Palladium(II).
Heating of a mixture of 2 and [PdCl2(MeCN)2] in toluene for
1 h gave an orange solution, from which a yellow solid of
formula [Pd2Cl2(C6F4PPh2)2] (11) was isolated in ca. 83% yield
(Scheme 1). The 31P NMR spectrum of 11 shows two broad
singlets at δ -77.4 and -76.7 whose relative intensity varies
in different preparations, indicating the presence of two species,
both of which clearly contain four-membered chelate rings; the
species responsible for the more shielded resonance is always
the more abundant. Traces of a third compound having a 31P
NMR singlet at δ 28.7 are also observed (see below). The far-
infrared spectrum of solid 11 shows two strong bands at 273
and 290 cm-1, which are not present in the spectrum of 2 and
can be assigned to the Pd-Cl stretching vibrations of a binuclear
Pd2(µ-Cl)2 unit.55,56 The corresponding bands for the closely
related, noncyclometalated complex [Pd2(µ-Cl)2(C6F5)2(P-
The 19F NMR spectra of 6-10 consist of the expected four
multiplets whose chemical shifts and assignments are similar
to those of their chelate precursors (Table 1). In each case, the
main difference from the spectra of 1-3 is that the resonance
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Ph3)2] appear at 270 and 290 cm-1 56
The data are consistent
.
with the isomeric chloro-bridged structures cis-11 and trans-
11 shown in Scheme 1; structure trans-11 has been confirmed
by X-ray crystallography.57 A structurally similar chloride-
bridged complex containing terminal cyclometalated [2-MeC6-
H4C6H3PtBu2]- ligands has also been reported recently.58
When a solution of 11 in CH2Cl2 was set aside at room
temperature, a yellow precipitate of the same composition as
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(54) Prive´r, S. H., unpublished work.
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(57) Rae, A. D.; Wagler, J., unpublished work.
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