H. Kunkely, A. Vogler / Journal of Organometallic Chemistry 577 (1999) 358–360
359
of this oxidative addition is Rh(PPh3)2(CS)Cl3. The
photolysis is monitored by measuring the decrease of
the optical density at 253 nm taking into account the
residual absorption of Rh(PPh3)2(CS)Cl3 at this wave-
length (m=8300). Rh(PPh3)2(CS)Cl disappears with
=0.003 at uirr=436 nm.
In CH3CN solutions Rh(PPh3)2(CS)Cl is hardly light
sensitive if oxygen is excluded. However, in the pres-
ence of O2 a photolysis takes place. The concomitant
spectral changes are similar but not identical to those
which are observed during the photolysis in CH2Cl2.
Fig. 1. Electronic absorption spectra of 8.06×10−5
M
RhI(PPh3)2(CO)Cl (a, ---) and 5.65×10−5 M RhI(PPh3)2(CS)Cl
3. Discussion
(b, —) in CH2Cl2 under argon at r.t, 1 cm cell.
In analogy to various other Rh(I) complexes [15–17]
with p-accepting ligands the longest-wavelength absorp-
tion of Rh(PPh3)2(CO)Cl at umax=364 nm has been
assigned to a MLCT transition which terminates at the
excitation may yield Rh(III) as a stable photooxidation
product. Finally, it should be useful to compare the
behavior of Rh(PPh3)2(CS)Cl with Rh(PPh3)2(CO)Cl.
The spectral [16,17] and photochemical [18–20] proper-
ties of the latter complex are well known.
phosphine
ligand
[16,17].
The
complex
Rh(PPh3)2(CS)Cl displays its lowest-energy band at dis-
tinctly longer wavelength (umax=452 nm) (Fig. 1). This
absorption is then logically assigned to the MLCT
transition from Rh(I) to the p* orbital of the thiocar-
bonyl ligand. This assignment is supported by related
observations on M(CO)5CS (M=Cr [11] and W [9,10])
and ReI(CO)4(S2COEt) [21].
Rh(PPh3)2(CO)Cl is well known to undergo a pho-
toejection of CO [18–20]. It seems likely that this
photodecarbonylation originates from a LF state in
agreement with the general behavior of metal carbonyls
[1–3]. Although LF bands are not apparent in the
spectrum of Rh(PPh3)2(CO)Cl they may be present at
relatively long wavelength but obscured by the more
intense MLCT absorption at 364 nm. Reactive LF
states can thus be populated from the MLCT state
which is initially reached by light absorption.
2. Results
The electronic spectrum of Rh(PPh3)2(CS)Cl in
CH2Cl2 (Fig. 1) shows absorptions at umax=452 (m=
1300 M−1 cm−1), 338 (4500), 290 (11300) and 253 nm
(sh, 25600). The spectrum is only slightly dependent on
the solvent. In CH3CN some band maxima are shifted
by
a
few nanometers. The absorptions of
Rh(PPh3)2(CO)Cl [16,17] in CH2Cl2 (Fig. 1) appear at
umax=364 (2800), 290 (12200) and 256 nm (18600).
Both complexes are not emissive at room temperature
(r.t.) or 77 K.
Solutions of Rh(PPh3)2(CS)Cl in CH2Cl2 are light
sensitive. The photolysis is accompanied by spectral
changes (Fig. 2) which can be duplicated by the thermal
reaction of Rh(PPh3)2(CS)Cl with Cl2 [13]. The product
The ML (p* CS) CT state of Rh(PPh3)2(CS)Cl is
located at rather low energies and apparently well
separated from higher LF states. The photoreactivity of
the complex is obviously initiated by MLCT excitation.
In CH2Cl2 a photoredox reaction takes place. It can be
described by the following equation:
RhI(PPh3)2(CS)Cl+2CH2Cl2
RhIII(PPh3)2(CS)Cl3+2 · CHCl2
Product formation may proceed in two steps. A pri-
mary electron transfer from the MLCT excited complex
to solvent leads to the generation of Rh(II) which is
subsequently oxidized by a second CH2Cl2 molecule in
a thermal process. One or two-electron photooxidations
of metal complexes by the solvent, in particular chlori-
nated alkanes, are frequently induced by MLCT excita-
tion [12,22]. As an alternative, in non-oxidizing solvents
such as CH3CN molecular oxygen may serve
as an oxidant. In this case the photoproduct of
Fig. 2. Spectral changes during the photolysis of 7.11×10−5
M
RhI(PPh3)2(CS)Cl in CH2Cl2 under argon at r.t. after 0 (a), 15 (b), 30
(c), 60 (d) and 120 (e) min irradiation time with uirr=366 nm (Xe/Hg
977 B-1 lamp), 1 cm cell.