Angewandte
Communications
Chemie
Then we turned our attention to the reaction mechanism.
was irradiated with blue LEDs in the presence of FCNIrpic.
We identified the segment of the substrate that interacts with
FCNIrpic by performing luminescence-quenching experi-
ments on 18 and 19, and comparing the results (Figure 2a):
the fluorescence of the photocatalyst FCNIrpic was quenched
by enaminone 18, while almost no quenching was observed
when FCNIrpic was mixed with indole 19. This indicates that
excited-state FCNIrpic activates the substrate solely by
interacting with the enaminone moiety. To prove that the
enaminone was activated via single electron oxidation[13a–p]
instead of energy transfer,[21] we synthesized compound 20,
and performed a comparative experiment (Figure 2b). It
shows that although the fluorescence of FCNIrpic could be
quenched by enaminone 20, no reaction occurred when 20
Conversely, when we irradiated enaminone 20 with a high-
pressure Hg lamp in the absence of FCNIrpic, the annulation
product 21 was obtained in 77% yield, indicating that once
triplet state 20* is formed, it should undergo [2+2]/retro-
Mannich-type process.[4a,14j] Thus, single electron oxidation
(20!20·+) is a more plausible explanation for the non-
productive luminescence-quenching. Electrochemical studies
performed in CH3CN also show that it is thermodynamically
feasible for the excited photocatalyst (Ep/2III*/II =+ 1.24 V vs.
Ag/AgCl) to oxidize substrate 14 (Ep/2ox =+ 1.18 V vs. Ag/
AgCl) via SET.
The reaction mechanism was further investigated compu-
tationally (Figure 3).[22] Stationary points for the organic
species were located at wB97M-V/def2-QZVP//
wB97X-D/def-TZVP level,[23] which was chosen
to better describe the radical-cation species.[24]
Rates and thermodynamic properties for SET
processes were estimated according to Marcus-
Hush theory using PBE0 functional with
LANL2TZ(f) basis set and pseudopotential for
Ir atoms and def-TZVP basis sets for others.[23d,25]
The functional was chosen to better describe the
transition-metal species.[26] SMD method was
used for solvation effects, including those
involved in external reorganization energies.[27]
The energies mentioned below are all Gibbs free
energies with solvation effects.
This reaction is probably initiated by single-
electron oxidation of substrate 14 to its radical
cation IM1 by excited-state FCNIrpic ([IrIII]*).
This process releases 1.1 kcalmolꢀ1 of free energy,
which is consistent with the electrochemical
analysis (DEox =+ 0.06 eV, ca. 1 kcalmolꢀ1). The
effective activation Gibbs free energy for the SET
process, was estimated to be a reachable 11.9 kcal
molꢀ1 according to the Marcus-Hush theory.
Electronic structure analysis confirmed that the
spin density of IM1 is located almost exclusively
at the enaminone moiety (see Supporting Infor-
mation), which is consistent with the lumines-
cence-quenching experiments.
Aided by a favorable p–p stacking interaction,
the oxidized enaminone moiety in IM1 readily
undergoes radical addition to the indole ring, with
a barrier of only 5.9 kcalmolꢀ1 (via TS1), to form
IM2. Subsequent addition of the benzylic radical
to the iminium moiety requires a barrier of
18.9 kcalmolꢀ1. The resulting radical-cation inter-
mediate IM3 is unstable and has a natural ten-
dency to either fragment back to IM2 (breaking
bond a) or forward to IM4 (breaking bond b). The
Figure 2. a) Luminescence-quenching experiments performed with 10 mM FCNIrpic
solution mixed with given concentration of 18 or 19. Substrate background was
measured with 0.025 molLꢀ1 of 18 or 19 without an Ir catalyst. b) Outcome of
control experiments and luminescence-quenching experiment result with 20. Both
reactions were performed in MeCN for 24 h at r.t. The quenching was measured
with 10 mM FCNIrpic solution mixed with given concentration of 20. Background
caused by direct excitation and florescence of 20 was subtracted from the spectrum
(see the Supporting Information).
regiochemistry of the fragmentation is coupled to
ꢀ
the out-of-plane bending vibration of the N H
ꢀ
bond; when N H vibrates so that the unbonded
single electron is mainly situated in a position
antiperiplanar to bond b (TS3, Figure 3), IM4 can
be readily reached, with a barrier of only 2.0 kcal
molꢀ1. IM4 can then be reduced by previously
Angew. Chem. Int. Ed. 2021, 60, 11211 –11216
ꢀ 2021 Wiley-VCH GmbH