1186
H. Kunkely, A. Vogler / Inorganic Chemistry Communications 8 (2005) 1185–1186
at 310 nm. The complex disappears with / = 0.007 at
irr = 520 nm.
k
The compound RuCl3(N2Ph)(PPh3)2 is a typical octahe-
dral d6 complex. LF absorptions are expected to appear at
wavelength not longer then 400 nm [10]. It follows that the
longest-wavelength band at kmax = 520 nm can be only
assigned to
a
RuðIIÞ ! Ph ꢀ Nþ2 MLCT transition.
Ru(II) ! NO+ transitions occur at comparable energies
[11]. MLCT excitation of RuCl3(N2Ph)(PPh3)2 in CH3CN
proceeds according to the simple scheme:
RuIICl3ðN2PhÞðPPh3Þ2 !RuIIICl3ðCH3CNÞðPPh3Þ2 þPhN2
ð1Þ
PhN2 !N2 þPh
2Ph!biphenyl
ð2Þ
ð3Þ
Fig. 1. Electronic absorption spectrum of 2.79 · 10ꢀ5 M RuCl3(N2Ph)-
(PPh3)2 in CH3CN under argon at room temperature, 1-cm cell.
The photolysis is certainly facilitated by the lability of the
phenyl diazonium radical as the primary photoproduct
which undergoes an irreversible decay.
In summary, we have shown that the aryldiazonium cat-
ion is a strong CT acceptor which is photooxidized to phe-
nyl radicals upon MLCT excitation. Various applications
including initiation of radical polymerization are
conceivable.
References
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Fig. 2. Spectral changes during the photolysis of 1.56 · 10ꢀ5 M
RuCl3(N2Ph)(PPh3)2 in CH3CN at room temperature after 0 min (a), 1,
2 and 6 min (b) irradiation times with kirr > 420 nm (Osram HBO 200 W/2
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of nitrogen gas bubbles. While RuCl3(N2Ph)(PPh3)2 is not
luminescent the photolyzed solution displays a blue emis-
sion at kmax = 305 nm with a shoulder at 315 nm which
indicates the formation of biphenyl [9]. The photolysis is
monitored by following the decrease of the optical density
[11] S.I. Gorelsky, A.B.P. Lever, Int. J. Quantum Chem. 80 (2000) 636
(and references cited therein).