138
H. Kunkely, A. Vogler / Inorganic Chemistry Communications 13 (2010) 137–138
Fig. 1. Spectral changes during the photolysis of 2.68 ꢁ 10ꢀ5
M
(pro-
phos)CuI(CO3)CuI(prophos) in acetonitrile at room temperature under argon at 0
(a), 15 and 40 min (b) irradiation times with kirr = 313 nm (Osram HBO 200 W/2
lamp), 1-cm cell.
Fig. 2. Potential energy diagram for the ground state and the lowest energy excited
states of (prophos)CuI(CO3)CuI(prophos).
variations including an isosbestic point at 231 nm (Fig. 1). During
irradiation of I is associated with an IL excitation. Partially, the
deactivation leads to an IL luminescence (kmax = 440 nm). The IL
emissions of comparable complexes [12] such as (P/3)2CuI(NO3)
at kmax = 450 nm [10] or [CuI(prophos)2]+ at kmax = 430 nm appear
in the same spectral region. Another deactivation path terminates
at a reactive ðCuI ! CO32ꢀÞ MLCT state which with participation of a
suitable vibration leads to the dissociation of CO from the carbon-
ate bridge (Fig. 2).
the photolysis
a continuous decrease of the absorption at
k > 231 nm takes place. The photoproduct shows a characteristic
spectrum (Fig. 1) with a maximum at 263 nm and further features
at kmax = 256, 271, 284 and 296 nm. Complex I displays a weak
luminescence at kmax = 440 nm (Fig. 2) which disappears during
the photolysis and is replaced by a much more intense lumines-
cence at kmax = 304 nm (Fig. 2). Further maxima appear at 282
(sh), 290 and 318 nm (sh).
According to this description the release of CO should be accom-
panied by the generation of a CuO2Cu moiety in the primary pho-
tochemical step. This fragment may contain CuIðO22ꢀÞCuI or its
redox isomer CuIIðO2ꢀÞ2CuII. Calculations have shown that they
are close in energy although such complexes are unknown
[13,14]. Since the CuO2Cu fragment should be quite oxidizing it
is not unexpected that it undergoes an oxygen transfer to a phos-
phine in agreement with our observation. It is well known that a
variety of oxygen transfer agents are able to convert phosphines
to phosphine oxides.
In summary, for the first time we describe the intramolecular
photoreduction of a carbonate ligand to CO. In addition, a phos-
phine ligand is transformed to a phosphine oxide as final oxidation
product. It is suggested that this photolysis is initiated by MLCT
excitation.
The absorption and emission spectrum of the photolyzed solu-
tion can be unambiguously attributed to 1,3-bis(diphenylphos-
phino)propane monoxide (prophos oxide, II) as shown by
comparison with the spectra of an authentic sample of II (ABCR,
Karlsruhe). From the difference of the extinction of II at 263 nm
(e = 4710) und 271 nm (e = 3768) its concentration can be deter-
mined reliably to some extent also in the presence of other absorb-
ing species provided they do not exhibit rather narrow absorptions
in this wavelength region. From the spectrum of the starting and
photolyzed solution equal molecular amounts of I and II are ob-
tained. The phosphine oxide II is formed with a quantum yield of
/ = 0.01 at kirr = 313 nm. Even at higher concentrations of I charac-
teristic LF bands of Cu(II) cannot be detected in the spectrum of the
photolyzed solution.
The photolysis of I is accompanied by the formation of a gas
which already in the beginning becomes visible as small bubbles.
This gas is not CO2. When it is introduced into an aqueous solution
of Na2CO3 which contains phenolphthalein as indicator the red
solution is not bleached by the formation of NaHCO3. The absorp-
tion of the red solution (kmax = 552 nm) remains unchanged. A gas
test specific for CO (gas detection pump accuro from Draeger
Safety) unambiguously shows that the gas formed during the pho-
tolysis of I is CO. This test can be also used for the quantitative
determination of CO but is less reliable at small amounts of gas.
In our case a molecular ratio of I to CO of 1:0.85 was obtained. In
addition, the gas volume was measured. For this purpose the pho-
tolysis was performed in a 3 ml cell which was connected to a gas
burette at constant pressure. The photolysis yielded a I to gas ratio
of 1:0.93 ( 5%). From these observations we conclude that the pho-
tolysis can be described by the simple stoichiometric equation:
Acknowledgement
Support of this research by the Deutsche Forschungsgemeins-
chaft (Grant No. VO 211/18-1) is gratefully acknowledged.
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CO2 þ prophos ! CO þ prophos monoxide
ð1Þ
On the basis of our observations and further considerations we
suggest that the photolysis proceeds by the following molecular
mechanism. In analogy to other Cu(I) phenylphosphine complexes
[12] including (P/3)2CuI(NO3) [10] the long-wavelength absorption
of I is attributed to an IL (phosphine) transition. Accordingly, the