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Table 1 IR-wavenumbers n~(CO) of 5a–d [in cmꢀ1
]
Remarkably, upon introducing a CH3- or CH3S-substituent (3d), the
frontier orbitals are destabilized compared to the reference com-
pound 3a, while especially the HOMO is now much higher in energy
than the HOMO in 3a. We believe that the rather strong +M effect of
especially the CH3S-group increases the p-donor properties of 3d by
conjugative interactions through the HOMO. This situation leads
consequently to an energetically high-lying HOMO and at the same
time to stronger p-donor properties. However, this does not clarify
why the IR-stretching frequencies in 5d are shifted to higher
wavenumbers compared to those in 5a. We anticipate that the
particular electronic properties of phosphinines might deliver a
plausible explanation: in contrast to common p-donor ligands, such
as halides, S2ꢀ or SCNꢀ (see the spectrochemical series), the LUMO
(p-accepting properties) and the HOMO (p-donating properties) in
3d have particularly large coefficients at the phosphorus donor-
atom, which are similar in shape and which point to the same
direction (Fig. 5). These molecular orbitals would therefore interact
with the same filled metal-centered d-orbital in an octahedral
complex, leading to repulsion and net weakening of the P–M bond
and, consequently, to a shift of the IR stretching modes to higher
wavenumbers, i.e. close to uncomplexed W(CO)6 (n~ = 1998 cmꢀ1).
We have demonstrated that the electronic properties of 2,4,6-
triarylphosphinine derivatives can be modulated systematically
and rather efficiently by introducing substituents into specific
positions of the heterocyclic framework. Furthermore, we found
evidence that the HOMO and HOMOꢀ1 of p-symmetry play a
significant role in the properties of metal complexes containing
s-coordinated phosphinine ligands, which has so far been
neglected for this class of compounds. This particular electro-
nic situation is caused by the special shape and orientation of
the LUMO and the HOMO of the phosphinine ligand and is
unique in comparison with other p-donors.
5a (–H)
5b (–F)
5c (–CF3)
5d (–SCH3)
n~1
n~2
n~3
n~4
2008
1893
1870
1836
2012
1893
1877
1840
2014
1920
n.d.
2014
1971
1889
1858
1857
marginal shift to higher wavenumbers compared to the reference
compound 5a (R = H). We attribute this minor increase in the
p-acceptor capacity of the phosphinine 3b to a +M effect of the
fluorine atom, which counterbalances the –I effect of this electron-
withdrawing substituent. Indeed, the IR-data of compound 5c,
which bears a –CF3 as a pure –I substituent in the para-position,
proved the higher p-accepting properties of ligand 3c. In the
presence of an electron-donating group in the same position of
the heterocycle, one would expect a shift to lower wavenumbers
due to an increased electron density in the antibonding p*(C–O)
orbitals. Much to our surprise, however, we clearly observed a
significant opposite effect for coordination compound 5d, which
contains a CH3S-substituent in the para-position. As a matter of
fact, we detected a considerable shift of the IR bands to higher
wavenumbers, rather than to lower ones. In order to explain this
unusual observation we carried out DFT-calculations at the B3LYP/
6-311+G(d,p) level on the pyridyl-functionalized phosphinines
3a–d and compared the relative energies of the frontier orbitals.
The results are depicted in Fig. 5. For comparison, we included
the H3C-substituted coordination compound in the calculations,
although the corresponding P,N-ligand could not be synthesized.8
Fig. 5 (right side) shows the shape of the frontier orbitals of the
CH3S-substituted phosphinine 3d. Qualitatively, both the sequence
and the shape of the p- and n-orbitals resemble the ones depicted
in Fig. 2 for the parent compound C5H5P with the exception that
the HOMOꢀ1 in C5H5P is now represented by the HOMOꢀ1 and
HOMOꢀ2 in 3d. This is also the case for phosphinines 3a–c. Upon
introducing a fluorine substituent (3b), the frontier orbitals are
slightly stabilized. This is in line with our chemical intuition that
the electron withdrawing fluorine substituent should lower the
energy of the LUMO which would consequently lead to stronger
p-accepting properties as observed also in the IR stretching
frequencies in 5b. This effect, however, seems to be only marginal
and might be attributed to the +M effect of the fluorine substituent.
The European Initial Training Network SusPhos (317404) is
gratefully acknowledged for financial support.
Notes and references
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¨
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8 Unfortunately, the pyrylium salt of the –CH3-substituted derivative
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`
9 A. Breque, C. C. Santini, F. Mathey, J. Fischer and A. Mitschler, Inorg.
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¨
Fig. 5 Frontier orbitals of 3a–d and the CH3-derivative.
8844 | Chem. Commun., 2014, 50, 8842--8844
10 J. Deberitz and H. Noth, J. Organomet. Chem., 1973, 49, 453.
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