Abstract:Hydrated electrons are super-reductants, yet can be generated with visible light when two photons are pooled, most efficiently through storing the energy of the first photon in a radical pair formed by the reduction of an excited catalyst by a sacrificial donor. All previous such systems for producing synthetically useable amounts of hydrated electrons with an LED in the visible range had to resort to compartmentalization by SDS micelles to curb the performance-limiting recombination of the pair. To overcome m… Show more
“…When HUr 2− is oxidized by the excited Ru II complex, it deprotonates and remains dianionic. Since the metal complex is also anionic in this case, Coulombic repulsion limits undesirable reverse electron transfer between the oxidized donor and the reduced photocatalyst, and consequently, the [Ru(dcob) 3 ] 4− /HUr 2− system enabled the micelle‐free production of synthetically useable amounts of hydrated electrons with an LED for the first time . Blue rather than green light was used to optimize the excitation process.…”
Section: The Next Level: Reductive Excited‐state Quenching Followed Bmentioning
The energy of visible photons and the accessible redox potentials of common photocatalysts set thermodynamic limits to photochemical reactions that can be driven by traditional visible‐light irradiation. UV excitation can be damaging and induce side reactions, hence visible or even near‐IR light is usually preferable. Thus, photochemistry currently faces two divergent challenges, namely the desire to perform ever more thermodynamically demanding reactions with increasingly lower photon energies. The pooling of two low‐energy photons can address both challenges simultaneously, and whilst multi‐photon spectroscopy is well established, synthetic photoredox chemistry has only recently started to exploit multi‐photon processes on the preparative scale. Herein, we have a critical look at currently developed reactions and mechanistic concepts, discuss pertinent experimental methods, and provide an outlook into possible future developments of this rapidly emerging area.
“…When HUr 2− is oxidized by the excited Ru II complex, it deprotonates and remains dianionic. Since the metal complex is also anionic in this case, Coulombic repulsion limits undesirable reverse electron transfer between the oxidized donor and the reduced photocatalyst, and consequently, the [Ru(dcob) 3 ] 4− /HUr 2− system enabled the micelle‐free production of synthetically useable amounts of hydrated electrons with an LED for the first time . Blue rather than green light was used to optimize the excitation process.…”
Section: The Next Level: Reductive Excited‐state Quenching Followed Bmentioning
The energy of visible photons and the accessible redox potentials of common photocatalysts set thermodynamic limits to photochemical reactions that can be driven by traditional visible‐light irradiation. UV excitation can be damaging and induce side reactions, hence visible or even near‐IR light is usually preferable. Thus, photochemistry currently faces two divergent challenges, namely the desire to perform ever more thermodynamically demanding reactions with increasingly lower photon energies. The pooling of two low‐energy photons can address both challenges simultaneously, and whilst multi‐photon spectroscopy is well established, synthetic photoredox chemistry has only recently started to exploit multi‐photon processes on the preparative scale. Herein, we have a critical look at currently developed reactions and mechanistic concepts, discuss pertinent experimental methods, and provide an outlook into possible future developments of this rapidly emerging area.
“…Wenn HUr 2− durch den angeregten Ru II ‐Komplex oxidiert wird, gibt es ein Proton ab und bleibt dadurch dianionisch. Die starke Coulomb‐Abstoßung schränkt den Rückelektronentransfer zwischen oxidiertem Donor und reduziertem Photokatalysator (beide anionisch) stark ein, wodurch das [Ru(dcob) 3 ] 4− /HUr 2− ‐System erstmals die mizellfreie Erzeugung syntheserelevanter e aq .− ‐Mengen mit einer LED ermöglicht . Um die Anregung zu optimieren, wurde blaues (statt grünes) Licht verwendet.…”
Section: Die Nächste Ebene: Reduktives Löschen Angeregter Zustände Gunclassified
Die Energie sichtbarer Photonen und die zugänglichen Redoxpotentiale üblicher Photokatalysatoren schränken die Anzahl derjenigen Photoreaktionen ein, die durch sichtbares Licht angetrieben werden können. Da UV‐Anregung schädlich ist und häufig Nebenreaktionen auslöst, ist sichtbares Licht oder sogar NIR‐Strahlung vorzuziehen. Die Photochemie befasst sich momentan mit einer zweischneidigen Herausforderung, und zwar mit dem Wunsch, immer thermodynamisch anspruchsvollere Reaktionen mit immer kleineren Photonenenergien durchführen zu können. Das Akkumulieren der Energie zweier energiearmer Photonen kann dazu passende Lösungsansätze liefern. Obwohl die Multiphotonen‐Spektroskopie gut etabliert ist, haben Photoredox‐Synthesechemiker erst kürzlich begonnen, Multiphotonen‐Prozesse präparativ zu nutzen. Hier werfen wir einen kritischen Blick auf kürzlich entwickelte Reaktionen und mechanistische Konzepte, diskutieren einschlägige experimentelle Methoden und geben einen Ausblick auf mögliche zukünftige Entwicklungen dieses jungen Forschungsgebiets.
“…However,i np hotochemistry one excited state quenched via photoinduced electront ransfer (PET) does not necessarily mean that one reduced or oxidized species is formed. Despite practically quantitative excited-state quenching, the actual yield of free radicals or radicali ons might be close to zero, [20,21] but the determinationo fc age-escape efficiencies h for ag iven PET event requires more sophisticated experimental techniques such as quantitative transienta bsorption spectroscopy.O wing to the lack of systematic quantitative studies in photochemistry,t he exact factorst hat govern the overall efficiencies of PET processes are stillp oorly understood and areliable predictiono fthe h values cannot be made in advance.F or instance, the inherent photoreduction efficiencies for an anionic ruthenium(II) complex by as eries of dianionic electron donors differ by as much as af actor of 30. [20] Most h values for PET reactions with triplet-excited Ru complexes are in the range from 0.05 (5 %) to 0.6 (60 %), [21][22][23][24][25][26][27] clearlyi ndicating that unproductive in-cage recombination is ag eneral energywasting problem.…”
One-electron reduced metal complexes derived from photoactive ruthenium or iridium complexes are important intermediates for substrate activation steps in photoredox catalysis and for the photocatalytic generation of solar fuels. However,o wing to the heavy atom effect, direct photochemical pathways to these key intermediates suffer from intrinsic efficiency problems resulting from rapid geminate recombination of radical pairs within the so-called solvent cage. In this study,w ep repared and investigated molecular dyads capable of producing reduced metal complexes via an indirect pathway relyingo nas equence of energy and electron transfer processes between aR uc omplex and ac ovalently connected anthracene moiety.O ur test reaction to establish the proof-of-concept is the photochem-ical reduction of ruthenium(tris)bipyridine by the ascorbate dianion as sacrificial donor in aqueous solution. The photochemicalk ey step in the Ru-anthracene dyads is the reduction of ap urely organic (anthracene) triplet exciteds tate by the ascorbate dianion, yielding as pin-correlated radical pair whose (unproductive) recombination is strongly spin-forbidden. By carrying out detailed laser flash photolysis investigations, we provide clear evidence for the indirect reduced metal complex generation mechanism and show that this pathway can outperform the conventionald irect metal complex photoreduction. The furthero ptimization of our approach involving relativelys imple molecular dyads might result in novel photocatalysts that convert substrates with unprecedented quantum yields.
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