P. Papadia et al. / Journal of Organometallic Chemistry 690 (2005) 2097–2105
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averaging for the two halves of the neocuproine ligand
due to fast rotation of the olefin on the NMR timescale
[2,14]. Interestingly, the DG# for the rotation of the
unsaturated ligand in these five-coordinate systems is
lower for palladium alkene or platinum alkyne neocupr-
oine complexes (DG# = 56.9 0.8 and 71.5 0.8
kJ molꢀ1 for [PdBr2(Me2phen)(g2-CH2@CHCH3)] [2]
and [PtI2(Me2phen)(g2-CH@CCH3)] [14], respectively).
Indeed, also in the case of complex 5 rotation around
the Pt–olefin bond must be a high energy process, since
two different sets of NMR signals, corresponding to the
two halves of the neocuproine ligand, are found. The se-
quence of 1H and 13C signals related to the two halves of
the neocuproine ligand was assigned on the basis of the
2D 1H NOESY and 2D [1H,13C]-HETCOR spectra.
Due to the presence of two diastereoisomers, a further
splitting for the signals was expected also for the neo-
group of neocuproine (3.40 ppm, Me(9) average value),
has NOE cross peaks only with @CH2 terminal protons
(4.012 and 3.955 ppm), while the deshielded signal
(3.43 ppm, Me(2) average value) has cross peaks only
with the @CHR terminal of the olefin (4.310 ppm)
(Fig. 3). The attribution of the neocuproine methyl sig-
nals allowed to assign the H3, H8 (7.776 and 7.772 ppm,
respectively) and the H4, H7 protons (8.254 and
8.263 ppm, respectively) of the phenanthroline (JH3–H4
and JH7–H8 = 8.3 Hz). The H5,6 protons (7.841 ppm)
gave a single resonance at the field used to acquire the
spectra. As for the iridium moiety, the 13C{1H} NMR
spectrum of the neocuproine ligand in complex 5 was as-
signed on the basis of the 2D [1H,13C]-HETCOR and
[1H,13C]-Long Range HETCOR spectra after the
sequential 1H assignment. In order to complete the
NMR characterization of compound 5, 1D 195Pt{1H}
NMR and [1H,195Pt]-HETCOR spectra were acquired.
Due to the large chemical shift range typical for 195Pt
NMR, diastereoisomeric platinum atoms often show
separate resonances [15]. Due to the quadrupole effect
of the chelate nitrogen ligand, the 1D 195Pt{1H} spec-
trum of 5 shows, for the two diastereoisomers, a broad
peak at d = ꢀ3889 ppm, which could be partially re-
solved in the [1H,195Pt]-HETCOR spectrum in two
peaks only 0.28 ppm apart from each other. The 195Pt
chemical shift values of the two diastereoisomers of 5
compare well with the chemicals shift at d =
ꢀ3893.10 ppm obtained for 6, suggesting a very similar
platinum coordination sphere for the two compounds,
which in the case of 5 does not seem to be affected by
the presence of the iridium moiety.
1
cuproine ligand. H and 13C NMR data of 5 show that
at the instrument field used (400 MHz) the only signals
of the neocuproine ligand showing different chemical
shift for the two diasteroisomers are those of the 2,9
methyls in the 1H NMR spectrum (two close signals
with an approximate 1:1 ratio at 3.437 and 3.434 ppm
for Me(2), 3.399 and 3.397 ppm for Me(9), respectively).
No doubling of the signals (1H,13C) due to the presence
1
of the two diastereoisomers was observed for H reso-
nances other than those of the neocuproine methyls,
most probably because of the distance of the chiral Ir
centre from the phenanthroline ring system. The 1:1
integral ratio observed for the two diastereoisomers
both for the neocuproine 2,9 methyl and the Me(30)
cyclopentadienyl signals, indicate that the presence of
a chiral center on the iridium atom does not give a sig-
nificant induction of chirality upon coordination of the
olefin to platinum. Due to the hindered rotation of the
3.6. Conformation of the Pt–Ir bridge complex 5
1
1
The 2D H NOESY spectrum also allowed to get
olefin bound to platinum, the 2D H NOESY spectrum
was particularly useful to assign the two halves of the
phenanthroline ligand, since dipolar couplings are
clearly and selectively seen between the Me(2) and
Me(9) with the @CHR and @CH2 vinylic protons,
respectively. In particular, the most shielded methyl
some information about the relative conformation in
solution for the two moieties of the Pt–Ir bridge com-
plex 5. In particular, among the two diastereotopic
allylic protons, one (Ha) seems to interact selectively
with the most deshielded of the two vinylic @CH2
=CH
2
cis trans
=CH-R
Me(9)
Me(2)
3.400
3.450
4.40
4.30
4.20
4.10
4.00
3.90
Fig. 3. 2D 1H NOESY spectrum of 5, expansion relative to the neocuproine methyl cross peaks with the vinylic protons of the iridium moiety.