posted on 2023-02-15, 16:34authored byAgustina Cotic, Simon Cerfontaine, Leonardo D. Slep, Benjamin Elias, Ludovic Troian-Gautier, Alejandro Cadranel
In natural and artificial photosynthesis, light absorption
and
catalysis are separate processes linked together by exergonic electron
transfer. This leads to free energy losses between the initial excited
state, formed after light absorption, and the active catalyst formed
after the electron transfer cascade. Additional deleterious processes,
such as internal conversion (IC) and vibrational relaxation (VR),
also dissipate as much as 20–30% of the absorbed photon energy.
Minimization of these energy losses, a holy grail in solar energy
conversion and solar fuel production, is a challenging task because
excited states are usually strongly coupled which results in negligible
kinetic barriers and very fast dissipation. Here, we show that topological
control of oligomeric {Ru(bpy)3} chromophores resulted
in small excited-state electronic couplings, leading to activation
barriers for IC by means of inter-ligand electron transfer of around
2000 cm–1 and effectively slowing down dissipation.
Two types of excited states are populated upon visible light excitation,
that is, a bridging-ligand centered metal-to-ligand charge transfer
[MLCT(Lm)], and a 2,2′-bipyridine-centered MLCT
[MLCT(bpy)], which lies 800–1400 cm–1 higher
in energy. As a proof-of-concept, bimolecular electron transfer with
tri-tolylamine (TTA) as electron donor was performed, which mimics
catalyst activation by sacrificial electron donors in typical photocatalytic
schemes. Both excited states were efficiently quenched by TTA. Hence,
this novel strategy allows to trap higher energy excited states before
IC and VR set in, saving between 100 and 170 meV. Furthermore, transient
absorption spectroscopy suggests that electron transfer reactions
with TTA produced the corresponding Lm•–-centered and bpy•–-centered reduced photosensitizers,
which involve different reducing abilities, that is, −0.79
and −0.93 V versus NHE for Lm•– and bpy•–, respectively. Thus, this approach
probably leads in fine to a 140 meV more potent reductant for energy
conversion schemes and solar fuel production. These results lay the
first stone for anti-dissipative energy conversion schemes which,
in bimolecular electron transfer reactions, harness the excess energy
saved by controlling dissipative conversion pathways.