.
Angewandte
Communications
allows a controlled delivery of reducing equivalents that
complexes are luminescent, with broad emissions centered at
618 nm (Supporting Information, Figure S4). The presence of
the Cu moiety leads to a 70% drop of the quantum yield in
II
overcomes the undesired Cu (O ) reduction.
2
3+
II
The [(bpy) Ru(bpbpa)Cu(OTf)(CH CN)] (bpy = 2,2’-
2
3
bipyridine, bpbpa = N-(4-((5H-dipyrido[3,2-c:2’,3’-e]azepin-
(7H)-yl)methyl)benzyl)-1-(pyridin-2-yl)-N-(pyridin-2-ylme-
thyl)methanamine) catalyst reported here, abbreviated as
air-equilibrated solution (from 1.05 ns to 0.29 ns) and 60%
under Ar (Supporting Information, Table S1). Previous
studies on comparable heteropolymetallic complexes featur-
6
II
II
2+
II
Ru phot-Cu
(Scheme 1, bottom), covalently associates
ing [Ru(bpy)3] and polypyridyl-Cu moieties ascribed the
cat
2+
a light-absorbing photosensitizing [Ru(bpy) ] -like frag-
emission quenching to either energy or electron transfer or
3
[
6]
[14]
ment, known to be an efficient chromophore, and a bio-
inspired copper site as the proposed catalytic oxidation locus.
It was efficiently prepared in two steps from the reported
both processes.
This point is discussed along with the
transient absorption spectroscopy. The lifetime decay for
II
Ru
is mono-exponential and air-sensitive, which is
phot
[
7]
[8]
3
[
(bpy) Ru(bpBr )][PF ] and l-NH -bpa precursors. The
characteristic of the MLCT excited state radiative decay
pathway (Supporting Information, Figure S5).
2
2
6
2
2
II
[13]
catalytic moiety (Cu cat) was synthesized from the l-Pht-bpa
protected ligand (Supporting Information, Scheme S1). The
syntheses and the characterization for all these compounds
The dyad
displays a bi-exponential lifetime decay with a short (16 ns in
air equilibrated solution and 31 ns under Ar) and a long
component (148–328 ns; Supporting Information, Figure S6).
By comparison with the mono-exponential decay determined
(
NMR and UV/Vis spectroscopy, elemental analysis, ESI-
MS) are provided in the Supporting Information. The nature
of the copper subunit coordination sphere is proposed on the
II
for Ru phot, the latter is ascribed to the radiative deactivation
II
3
basis of the X-ray crystal structure resolved for Cu cat
of MLCT excited state. Considering i) that energy transfer
(
Supporting Information, Figure S1).
The cyclic voltammogram (CV) of Ru phot-Cu
between the triplet excited state of the ruthenium and the
singlet ground state of the copper moieties is a spin-forbidden
process; ii) that the weak extinction coefficient of the Cu
subunit makes energy transfer a possible but likely minor
II
II
cat
in
CH CN shows, in the cathodic region, three successive one-
3
electron processes between À0.7 and À1.7 V vs NHE
[14b,15]
corresponding to the reduction of the bipyridine ligands
component of the excited state quenching;
and iii) the
II
3
(
Supporting Information, Figure S2). Surprisingly, three
estimated redox potential of Ru * MLCT excited state
[10b]
II
waves were observed in the anodic region. On the basis of
previous reports and CVs recorded for Cu
(
(À0.70 V vs NHE ) and the redox potential of Cu
II
and [(bpy) Ru-
(+ 0.42 V vs. NHE), the quenching is most likely due to an
cat
2
2+
II
II 3
bpbpa)] metalloligand (abbreviated Ru phot), the two one-
electron transfer from the Ru MLCT excited state to the
II
[14c,16]
electron quasi-reversible waves at + 1.57 V and + 0.42 V vs
Cu moiety (as early observed
). Consequently, the short
III
II[9]
II
I
NHE were attributed to the Ru /Ru and Cu /Cu couples,
respectively (Supporting Information, Figure S2). Thermody-
namically, by considering the redox potential of the excited
lifetime is ascribed to the decay of the excited state quenched
by photoinduced electron transfer (PET). The corresponding
7
À1
rate, estimated to be 2.9 10 s in argon equilibrated
III
II
[10]
II
II
state of the Ru subunit(E8 Ru /Ru *) of À0.70 V vs NHE,
acetonitrile solution for Ru phot-Cu , is artificially increased
cat
II
7
À1
an electron transfer from the photoexcited state Ru * to the
in air-equilibrated medium (5.6 10 s ), owing to the addi-
tional quenching by energy transfer to the triplet ground state
of molecular oxygen. The presence of triethanolamine
(TEOA, sacrificial electron donor) in the catalytic conditions
slightly affects the spectroscopic properties (Supporting
Information, Table S1, Figures S3, S4, and S6). All these
results enforce the viability of an electron transfer from the
II
Cu is consequently favorable. The third irreversible oxida-
tion process at + 1.44 V vs. NHE (anodic peak given) was
assigned to the oxidation of the tertiary amine of the bridging
ligand (N , Scheme 1).
comparison with the metal-free bdda molecule (Supporting
Information, Scheme S1, Figure S2) showing a similar irre-
versible pattern with an anodic peak at + 1.40 V vs. NHE.
The reliability of the photocatalytic system based on an
intramolecular electron transfer between the excited Ru
moiety and the vicinal Cu center was probed by EPR and
photophysical studies. The photophysical properties of
[11]
This was further confirmed by
A
[
12]
II
II
excited Ru *
to the Cu cat, rather than a reductive
phot
II
quenching of the Ru *
by the electron donor (Supporting
phot
Information, Scheme S2).
The photo-assisted Cu reduction in Ru
catalytic conditions (that is, CH CN, [Ru phot-Cu cat] = 10 m,
II
II
phot
II
-Cu
under
cat
II
II
À4
3
II
II
II
cat
Ru
and Ru phot-Cu
have been investigated in CH CN
TEOA 200 molar equiv) was probed under Ar-saturated
atmosphere by EPR spectroscopy. Spectra were recorded
before (t = 0 min), and after 1 and 5 min of irradiation with
a Xe lamp equipped with a by-pass filter at 450 nm (Figure 1).
At t = 0 min, the EPR spectrum is characteristic of
phot
3
at room temperature, both in air equilibrated and de-aerated
conditions (Supporting Information, Table S1). Both com-
plexes display an intense absorption around 290 nm (e =
À1
À1
À1
À1
II
6
0500 Lmol cm and e = 56 800 Lmol cm for Ru
phot
II
II
and Ru phot-Cu cat, respectively) assigned to p–p* transitions
Supporting Information, Figure S3). The broad absorption
bands around 445 and 455 nm are attributed to the metal-to-
a mononuclear copper center in axial symmetry (g > g )
k ?
(Support-
cat
II
(
with identical features compared to isolated Cu
[17]
ing Information, Figure S7). Upon light exposure of the
dyad in the ruthenium MLCT transition region at 298 K, the
EPR signal rapidly decreased and completely vanished within
1
[13]
ligand charge transfer transition ( MLCT, dp –p*bpy). It is
worth noting that the Cu-centered d–d transitions for the
dyad are not observable owing to their weak extinction
coefficient (lmax = 615 nm and e = 100 Lmol cm
Cu
Ru
II
45 min. A complete recovery of the Cu features was
À1
À1
for
observed upon exposure to air. The decomposition of the
dyad has to be precluded, as confirmed by the full conserva-
II
Cat
; Supporting Information, Figure S3). Upon excitation
II
II
II
cat
II
in the MLCTabsorption band, both Ru phot and Ru phot-Cu
tion of the UV features after 45 min of irradiation of Ru phot-
8
416
ꢀ 2015 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2015, 54, 8415 –8419