Noble-Metal-Free Photocatalytic Hydrogen Production from Water
FULL PAPER
unprecedentedly high values of up to 54.1 ms and 74.5%, re-
spectively (for complex 3; Table 1, entry 3). These high
values are more astonishing considering the fact that the
measurements were performed in THF, which, as a Lewis
base, can typically act as an additional ligand.[23]
These results reflect the effective shielding of the metal
core that is imparted by the bulky ligands. For both proper-
ties, t0 and Fabs, the same trend is observed within series of
complexes 1–3 and 7–9 (that is: 1<2<3 and 7<8<9) and,
not surprisingly, it is derived from the ability with which the
flattening distortion of the cupric excited state is inhibited
(perfectly correlated with the bulkiness of the substituents:
Me<nBu<sBu). Under catalytic conditions (with a higher
concentration of PS and in the presence of TEA and water),
much shorter lifetimes (tcat, Table 1) were observed (see
below).
Figure 3. Cyclic voltammograms of complexes 1 (red), 3 (green), and 7
(blue) in MeCN solution. All potentials are referenced to the Fc/Fc+
couple. Inset: Oxidative differential pulse voltammograms (DPVs). Scan
, supporting electrolyte: 0.1m [Bu4N]PF6, Ag/AgCl/
LiClsat. reference electrode, glassy carbon working electrode, platinum
Upon excitation, the formally 3d9 metal center tends to
adopt a pseudo-square-planar geometry with two open coor-
dination positions in which one or two solvent molecules
can coordinate to form an exciplex intermediate.[23] This spe-
cies has a smaller energy gap to the ground state and, conse-
quently, the non-radiative decay pathway is favored; thus,
short lifetimes of the MLCT state are observed.[24] Effective
inhibition of this process, as in our case, leads to long-lived
excited states (with high-energy levels), along with high
quantum yields. The experimentally measured lifetimes (t0)
and quantum yields (Fabs, Table 1) were used to calculate
the radiative (kr) and non-radiative rate constants (knr) of
the MLCT excited states (see the Supporting Information,
Table SI1).[25] The obtained kr values are typical of hetero-
leptic copper complexes with phenanthroline and diphos-
phine ligands.[21] Conversely, the obtained knr values are up
to three orders of magnitude smaller than those for homo-
leptic phenanthroline complexes,[26] which indicates that the
non-radiative decay is much slower and accounts for the rel-
ative long lifetimes of the excited states, thus fulfilling one
of the prerequisites for a complex to be a successful photo-
sensitizer for solar-energy-conversion systems.
rate: 100 mVsÀ1
counter electrode, temperature: 258C.
Table 2. Electrochemical data of selected complexes in MeCN.[a]
Entry
Complex
Eox [V]
Ered [V]
DEoxÀred [V]
1
2
3
1
3
7
+0.93
À2.05
À2.12
À2.03
2.98
+1.02
3.14
+0.90 (+1.08)[b]
2.93 (3.11)[b]
[a] The measurements were carried out in dry MeCN under an argon at-
mosphere with 0.1m [Bu4N]PF6 as a supporting electrolyte. Peak poten-
tials are versus Fc/Fc+ (for potentials versus NHE and Ag/AgCl see the
Supporting Information, Table SI2)
phine ligand is oxidized, presumably at the sulfur atom. Be-
sides this peak, the substitution pattern in complex 3 causes
an oxidation potential that is 90 mV higher than that of
complex 1.
Because differences in the electronic inductive effects be-
tween the alkyl groups cannot be invoked, the shift in the
oxidation potentials should be attributed to the larger steric
effect of the sec-butyl group (in 3) compared to the methyl
group (in 1), thus more-effectively preventing the structure-
flattening that is associated with the oxidation of CuI to CuII
and, hence, stabilizing the cuprous state.[16b,21,27] Conversely,
the effect of the 2,9-substitution pattern cannot be observed
in the absorption spectra (Figure 2), because the spectra are
not influenced by structural changes that occur after the
MLCT process.[21]
Electrochemical studies: For complexes 1, 3, and 7, cyclic
and differential pulse voltammograms were recorded in
MeCN solution (Figure 3 and Table 2). Upon reduction, all
of the complexes display comparable behavior, with a rever-
sible single-electron-reduction couple. This peak is associat-
ed with a reduction of the phenanthroline ligand and, thus,
_
_
CÀ
with the formation of [CuII
known from previous studies of related [Cu
A
N
It is important to mention that, as previously reported for
_
A
[CuACTHUNGETRNNUG
(NN)2]+ complexes,[21] the oxidation process is not totally
plexes.[21] Comparing the reduction potentials of complexes
1 (À2.05 V) and 3 (À2.12 V versus Fc/Fc+), a shift of about
70 mV is observed, thus indicating an influence of the substi-
tution pattern at the 2- and 9-positions of the phenanthro-
line scaffold. In contrast, the influence of different phos-
phine ligands is negligible, as shown by complexes 1 and 7,
which only display a small difference of 30 mV between
their metal-based oxidation potentials (0.93 and 0.90 V
versus Fc/Fc+, respectively). Moreover, for complex 7,
a second oxidation peak can be observed, in which the phos-
reversible (Figure 3), because DEoxÀred also incorporates
energy changes that are associated with structural modifica-
tions (Jahn–Teller distortion and coordination number). For
the same reason, a direct correlation between the emission
energies and the reduction potentials (expected for d6 metal
complexes) is not observed.[28]
Nevertheless, the reduction and oxidation potentials of
the excited states can be calculated from their corrected
emission energies; that is, instead of the emission maxima,
the values that are obtained from the intersection of the
Chem. Eur. J. 2013, 19, 15972 – 15978
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15975