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. 2022 Jul 20;13(32):9165–9175. doi: 10.1039/d2sc02122f

Excited state reactions in the cycle shown in Scheme 3 (KSV = Stern–Volmer quenching rate, kq = bimolecular rate constant, ηq = quenching yield, ηce = cage escape yield, ηqηce = quantum yield)a.

PS (τ0/ps)
[Fe(iii)(btz)3]3+, 1 (94) [Fe(ii)(btz)3]2+, 2 (330)
K SV/M−1 k q/109 M−1 s−1 η q ([Q]/M) η ce η q η ce ([Q]/M)
TEA 0.81b 8.4 0.31 (0.50) 0.29c 0 (≤0.50)d
C8F17I n.a.e n.a. 0 (≤0.45)f n.a. 0.18c (0.45)g,h
5-Hexen-1-ol n.a. n.a. 0 (≤0.14)f n.a. 0 (≤0.14)d
a

In MeCN : MeOH (4 : 3).

b

Stern–Volmer constant from steady state emission quenching.

c

±20%.

d

No detectable products in ns-transient absorption.

e

Not applicable.

f

No emission quenching up to indicated quencher concentration.

g

From ns-transient absorption.

h

η ce ≥ 0.3 with ηq(0.45 M) ≤ 0.6 (based on kq ≤ 2 × 1010 M−1 s−1).