10.1002/anie.202009704
Angewandte Chemie International Edition
kcal·mol-1 (Figure S6, C). We also discovered an alternative lower
energy pathway that could operate in the presence of water (5.7
kcal·mol-1, Figure 1C). In this scenario, the water co-solvent acts to
shuttle a proton from C9a to C2 leading to the product. However, when
a base such as AcONa is used or the concentration of water as a
cosolvent is low, other pathways might become the preferred routes
to promote this 1,3-shift (Figure S6, C and D).
In conclusion, we have discovered an operationally simple and
functional group tolerant synthesis of pyrroloindoles that proceeds in
the presence of visible light and an iridium(III) sensitizer. The
reaction proceeds via cyclization in the triplet excited state to yield a
1,4-diradical; intersystem crossing leads preferentially to a closed
shell singlet zwitterion that is geometrically restricted from
undergoing recombination to yield a cyclobutane, leading to the
preferential formation of a 5,5-bicyclic lactam ring system.
To probe the practical utility of this transformation, a gram
scale synthesis of 6-bromo substrate 14 was performed. By starting
with 4.6 mmol of the appropriate precursor, 1.39 g of 14 were
obtained (93%), thus demonstrating that the reaction is scalable
without affecting the overall yield.
In order to probe the mechanistic profile of this transformation,
we carried out computational studies with density functional theory
(DFT,12 M06-2X-D3/Def2-QZVPP//M06-2X-D3/6-31++G(d,p);13-15
in SMD ethyl acetate)16 in conjunction with experimental techniques
(Figure 1). The calculated energy required to promote N-acyl 1A from
the singlet (S0) to p-p* triplet (T1) state is 52.2 kcal·mol-1. This is
well matched with the emissive energy of the Ir(dFppy)3 (60.1
kcal·mol-1)17, [Ir(dF(CF3)ppy)2(dtbbpy)]PF6 (61.8 kcal·mol-1)17 and
fac-Ir(ppy)3 (55.2 kcal·mol-1)17 catalysts. To exclude an alternative
photoredox catalytic cycle, we turned our attention to electrochemical
studies. Square voltammetry performed on substrate 1 indicated a
reduction potential of -1.62 V and an oxidation potential of 1.91 V
(vs SCE in MeCN). Both reduction and oxidation potentials are
outside the redox capabilities of the optimal Ir(dFppy)3 catalyst
(E1/2(M+/M*) = -1.27 V; E1/2(M*/M-) = 0.35 V vs SCE in MeCN).17
Furthermore, Stern-Volmer quenching experiments showed a clear
substrate catalyst interaction, thus making energy transfer the most
probable mechanistic candidate.
Received: ((will be filled in by the editorial staff))
Published online on ((will be filled in by the editorial staff))
Keywords: visible light • photochemistry • mechanism • energy
transfer • catalyst • DFT
Our proposed mechanism is pictured in Figure 1. After singlet-
to-triplet excitation of the initial substrate by the excited state catalyst
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1
and generates the corresponding singlet species B; this species is
better described as a closed-shell singlet zwitterion rather than a
singlet diradical (⟨ Ŝ2 ⟩ = 0 in the wavefunction stability checks). This
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with the pyrroloindole product, consistent with the presence of an
enolate-like intermediate. The last step of the proposed mechanism
involves transformation of the zwitterion 1B into the final product C.
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C9a of 1B to C2. To probe this, we subjected deuterated substrate 33
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(Figure 1C). Under these conditions only a small amount of
deuterium in the C2 position was observed in 34. This result implies
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using D2O as co-solvent with a non-deuterated indole 1, the C2
position of product 35 showed significant deuterium incorporation
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2 is unreactive under these conditions and no deuterium incorporation
is observed. This is consistent with a pathway whereby the C2
hydrogen comes from solvent. We probed this with further
calculation and found that the stepwise solvent mediated
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4
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