Angewandte
Communications
Chemie
Photocatalysis Very Important Paper
Sensitization-Initiated Electron Transfer for Photoredox Catalysis
Abstract: Photosynthetic organisms exploit antenna chromo-
phores to absorb light and transfer excitation energy to the
reaction center where redox reactions occur. In contrast, in
visible-light chemical photoredox catalysis, a single species
(i.e., the photoredox catalyst) absorbs light and performs the
redox chemistry. Mimicking the energy flow of the biological
model, we report a two-center photoredox catalytic approach
in which the tasks of light energy collection and electron
transfer (i.e., redox reactions) are assigned to two different
molecules. Ru(bpy)3Cl2 absorbs the visible light and transfers
the energy to polycyclic aromatic hydrocarbons that enable the
redox reactions. This operationally simple sensitization-initi-
ated electron transfer enables the use of arenes that do not
absorb visible light, such as anthracene or pyrene, for photo-
redox applications. We demonstrate the merits of this approach
by the reductive activation of chemical bonds with high
reduction potentials for carbon–carbon and carbon–hetero-
atom bond formations.
times and relatively poor photochemical quantum yields, the
restricted redox energy gain upon visible-light photoexcita-
tion limits the overall performance of a photoredox catalyst
with respect to the substrate scope. Furthermore, in accord-
ance with the common notion that the more reductive
a catalyst, the less oxidative it is, synthetically demanding
chemical modifications enhance the redox equivalence gain in
one direction at the expense of the other (oxidative/reductive
or vice versa).[9]
Inspired by the natural photosynthetic systems, we
envisioned using strongly absorbing molecules for light
energy harvesting and funneling the excitation energy to
a highly reducing molecule that does not absorb visible light.
The redox potential of the latter species may be utilized to
drive challenging redox reactions that are not feasible or less
efficient with a single photocatalyst. The effective conversion
of visible-light energy into redox equivalents in different
photoredox catalytic systems is compared in Scheme 1. The
energies of blue (455 nm) and green photons (530 nm) of
262 kJmolÀ1 or 2.72 eV and 226 KJmolÀ1 or 2.34 eV, respec-
tively, are insufficient for the activation of many chemical
bonds via direct photoexcitation. However, converting the
same energy into redox equivalents enables the activation of
such bonds through single-electron-transfer redox processes.
The many applications of visible-light photoredox catal-
ysis for the activation of chemical bonds that have been
reported over the last decade document the practicality of
such energy transduction processes.[3–7,10] However, as the
electronic rearrangements of the photoredox catalysts upon
light absorption commence the energy transduction process-
es, the intrinsic properties, in particular, the absorption and
ground-state redox potentials of the photoredox catalysts,
define how much light energy can be converted into redox
energy (Rehm–Weller equation).[11] As depicted in Scheme 1,
the maximum reduction potential available in a typical
Ru(bpy)32+-based photoredox catalytic system never exceeds
a value of À1.33 V (the inherent ground-state reduction
P
hotosynthetic organisms transform light energy into chem-
ical free energy through a series of energy-transducing
reactions. Visible light is harvested by antenna pigments,
such as chlorophyll b and b-carotene, and transferred to the
reaction center pigment, chlorophyll a, to drive photosyn-
thetic reactions.[1–2] This strategy of using strongly absorbing
antenna molecules for visible-light collection and weakly
absorbing redox centers to drive chemical reactions enables
the efficient conversion of light energy into redox energy for
the simultaneous oxidation of water to molecular oxygen and
the reduction of NADP+ to NADPH. In contrast, visible-
light-mediated photoredox catalysis,[3–7] an emerging field in
synthetic organic chemistry, uses visible light to drive
chemical reactions, but relies on the use of the same molecule
(i.e., a photoredox catalyst) for both visible-light absorption
and the conversion of the light energy into redox energy to
initiate redox reactions. This excludes the application of many
chromophores that have extremely high redox potentials, but
do not absorb visible light (e.g., polycyclic aromatic hydro-
carbons for reduction reactions; c.f., sodium naphthalenide)
in photoredox catalysis, and leads to a strong dependence on
the inherent redox potentials of typical photoredox catalysts
for the conversion of visible light into the maximum available
redox energy.[8] Aside from the typically very long reaction
+
potential of Ru(bpy)3 ).[3] In contrast, the photoredox cata-
lytic approach based on sensitization-initiated electron trans-
fer (SenI-ET) uses the intrinsic properties (absorption and
redox potentials) of two different molecules for the con-
version of light energy into redox energy through a bimolec-
ular energy-transfer process. Here, although the energy of
visible light is insufficient to access the excited states of the
redox-active species (the DE for photoexcitation), the relative
energy of its excited state with respect to the visible-light-
absorbing sensitizer allows its excitation via a simple photo-
induced energy-transfer process. As depicted in Scheme 1,
such an energy transduction allows accessing the reduction
potentials of polycyclic aromatic hydrocarbons, such as
pyrene or anthracene. Even more interestingly, the reduction
potentials of the radical anions of the polycyclic aromatic
[*] Dr. I. Ghosh, Dr. R. S. Shaikh, Prof. Dr. B. Kçnig
Universitꢀt Regensburg
Fakultꢀt fꢁr Chemie und Pharmazie
93040 Regensburg (Germany)
E-mail: burkhard.koenig@ur.de
Supporting information and the ORCID identification number(s) for
Angew. Chem. Int. Ed. 2017, 56, 1 – 7
ꢀ 2017 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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