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Protein aggregation into amyloid fibrils underlies numerous human diseases, yet the most widely used fluorescent probe, Thioflavin T (ThT), offers an incomplete picture of the process and fails to detect certain fibril structures. Here, we introduce and characterize the photophysical properties of DANIR-2b(2OH), a water-soluble push–pull dye that overcomes these limitations. It successfully binds early prefibrillar aggregates and small fibrils of the human Islet Amyloid Polypeptide that elude detection by ThT, which we confirm by time-resolved cryo-electron microscopy of aliquots taken during the kinetic assays. We further demonstrate that DANIR-2b(2OH) can also track the aggregation of other amyloid proteins, such as insulin and Aβ_1–42. The protein-dye interaction was characterized via steady-state and time-resolved fluorescent spectroscopy. DANIR-2b(2OH) features environment-sensitive emission, high photostability, and a straightforward synthesis. Critically, it provides a substantially lower noise level in standard plate-reader assays, allowing the tracking of aggregation processes that are not visible in standard ThT measurements. This establishes DANIR-2b(2OH) as a highly sensitive and broadly applicable probe for real-time amyloid aggregation measurements and imaging.

A ferrous complex bearing tris(carbene)borate ligands with imidazol-2-ylidene donors has been characterized by experimental and computational methods. Despite the pronounced destabilization of metal centered states by the exceptionally σ-donating ligand, the high-energy 3MLCT state of [Fe(II)(phtmeimb)2] is rapidly deactivated by the barrierless conversion to the 3MC state.

[Ru(bpy)₃]²⁺, tris(bipyridine)ruthenium(II), is a popular transition metal complex whose favorable photophysical properties have afforded it a central place in inorganic photochemistry and various related fields. In this perspective, in contrast to the large number of extant technical reviews, we instead note critical developments from a historical context. Of particular note are relatively lesser-known investigations in the field of analytical chemistry that predate the complex’s rise to prominence as a photosensitizer. Recent studies that revisit the complex’s own fundamental photophysics are also highlighted. Thus, in addition to serving as a proverbial almanac for the complex’s rich history, this condensed perspective portends yet more fruitful lives for research into [Ru(bpy)₃]²⁺, despite the many already lived.

A series of 2,1,3-benzothiadiazole–Au(I)–L complexes have been synthesised, structurally characterised and investigated for their photophysical properties. These are the first organometallic Au(I) complexes containing a C–Au bond on the highly electron-deficient benzothiadiazole unit. The complexes exhibit solution-phase phosphorescence at room temperature, assigned to the intrinsic triplet state of the benzothiadiazole unit that is efficently populated through its attachment to gold. Comparison with routinely reported Au(I) complexes, which include intervening alkenyl linkers, suggests that previous assignments of their phosphorescence as ¹π → π*(CCR) might be incomplete. Our observations affirm that, in addition to the heavy atom effect, breaking symmetry in the involved aryl motif may be of importance in controlling the luminescence properties.

Detailed photophysical investigation of a Mn(IV)-carbene complex has revealed that excitation into its lowest-energy absorption band (∼500 nm) results in the formation of an energetic ligand-to-metal charge-transfer (LMCT) state with a lifetime of 15 ns. To the best of our knowledge, this is the longest lifetime reported for charge-transfer states of first-row-based transition metal complexes in solution, barring those based on Cu, with a d¹⁰ configuration. A so-called superoxidant, Mn(IV)-carbene exhibits an excited state potential typically only harnessed via excited states of reactive organic radical species. Furthermore, the long-lived excited state in this case is found to be a dark doublet, with its transition to the quartet ground state being spin-forbidden, a contrast to most first-row literature examples, and a possible cause of the long lifetime. Showcasing excited state properties which in some cases exceed those of complexes based on precious metals, these findings not only advance the library of earth-abundant photosensitizers but also shed general insight into the photophysics of d³ and related Mn complexes.

Two iron complexes featuring the bidentate, nonconjugated N-heterocyclic carbene (NHC) 1,1′-methylenebis(3-methylimidazol-2-ylidene) (mbmi) ligand, where the two NHC moieties are separated by a methylene bridge, have been synthesized to exploit the combined influence of geometric and electronic effects on the ground- and excited-state properties of homoleptic Fe^III-hexa-NHC [Fe(mbmi)₃](PF₆)₃ and heteroleptic Fe^II-tetra-NHC [Fe(mbmi)₂(bpy)](PF₆)₂ (bpy = 2,2′-bipyridine) complexes. They are compared to the reported Fe^III-hexa-NHC [Fe(btz)₃](PF₆)₃ and Fe^II-tetra-NHC [Fe(btz)₂(bpy)](PF₆)₂ complexes containing the conjugated, bidentate mesoionic NHC ligand 3,3′-dimethyl-1,1′-bis(p-tolyl)-4,4′-bis(1,2,3-triazol-5-ylidene) (btz). The observed geometries of [Fe(mbmi)₃](PF₆)₃ and [Fe(mbmi)₂(bpy)](PF₆)₂ are evaluated through L–Fe–L bond angles and ligand planarity and compared to those of [Fe(btz)₃](PF₆)₃ and [Fe(btz)₂(bpy)](PF₆)₂. The Fe^II/Fe^III redox couples of [Fe(mbmi)₃](PF₆)₃ (−0.38 V) and [Fe(mbmi)₂(bpy)](PF₆)₂ (−0.057 V, both vs Fc^+/0) are less reducing than [Fe(btz)₃](PF₆)₃ and [Fe(btz)₂(bpy)](PF₆)₂. The two complexes show intense absorption bands in the visible region: [Fe(mbmi)₃](PF₆)₃ at 502 nm (ligand-to-metal charge transfer, ²LMCT) and [Fe(mbmi)₂(bpy)](PF₆)₂ at 410 and 616 nm (metal-to-ligand charge transfer, ³MLCT). Lifetimes of 57.3 ps (²LMCT) for [Fe(mbmi)₃](PF₆)₃ and 7.6 ps (³MLCT) for [Fe(mbmi)₂(bpy)](PF₆)₂ were probed and are somewhat shorter than those for [Fe(btz)₃](PF₆)₃ and [Fe(btz)₂(bpy)](PF₆)₂. [Fe(mbmi)₃](PF₆)₃ exhibits photoluminescence at 686 nm (²LMCT) in acetonitrile at room temperature with a quantum yield of (1.2 ± 0.1) × 10^–4, compared to (3 ± 0.5) × 10^–4 for [Fe(btz)₃](PF₆)₃.

Direct excitation of aromatic compounds grants access to high-energy intermediates that can be utilised in organic synthesis. Understanding and predicting the substituent effects at the excited state for aromatic molecules remains challenging for the synthetic photochemist. In this work, we present an experimental and computational investigation of the excited state of the isomeric chloroanilines, which promptly react by losing the chloride when the amino group is in para position, but are non-reactive and non-emissive in the meta and ortho isomers. XMS-CASPT2//CASSCF computations explain this apparent contradiction of the meta-ortho selectivity rule of Zimmerman, which originates from the substituent effects lowering to a different extent the barrier to populate the prefulvenic conical intersection that deactivates non-radiatively the singlet excited state of the chloroanilines. Computational chemistry allows to elucidate the observed selectivity in the photochemistry of chloroanilines. A meta-ortho effect of the substituents favours the population of the prefulvenic conical intersection which leads to rapid deactivation of the m- and o-isomers of chloroaniline, while the para derivative lives long enough to emit and populate the reactive triplet state which leads to C-Cl dissociation.+image

We show here that soap films-typically expected to host symmetric molecular arrangements-can be constructed with differing opposite surfaces, breaking their symmetry, and making them reminiscent of functional biological motifs found in nature. Using fluorescent molecular probes as dopants on different sides of the film, resonance energy transfer could be employed to confirm the lack of symmetry, which was found to persist on timescales of several minutes. Further, a theoretical analysis of the main transport phenomena involved yielded good agreement with the experimental observations.

We here report the synthesis of the homoleptic iron(II) N-heterocyclic carbene (NHC) complex [Fe(miHpbmi)(2)](PF6)(4) (miHpbmi = 4-((3-methyl-1H-imidazolium-1-yl)pyridine-2,6-diyl)bis(3-methylimidazol-2-ylidene)) and its electrochemical and photophysical properties. The introduction of the pi-electron-withdrawing 3-methyl-1H-imidazol-3-ium-1-yl group into the NHC ligand framework resulted in stabilization of the metal-to-ligand charge transfer (MLCT) state and destabilization of the metal-centered (MC) states. This resulted in an improved excited-state lifetime of 16 ps compared to the 9 ps for the unsubstituted parent compound [Fe(pbmi)(2)](PF6)(2) (pbmi = (pyridine-2,6-diyl)bis(3-methylimidazol-2-ylidene)) as well as a stronger MLCT absorption band extending more toward the red spectral region. However, compared to the carboxylic acid derivative [Fe(cpbmi)(2)](PF6)(2) (cpbmi = 1,1 '-(4-carboxypyridine-2,6-diyl)bis(3-methylimidazol-2-ylidene)), the excited-state lifetime of [Fe(miHpbmi)(2)](PF6)(4) is the same, but both the extinction and the red shift are more pronounced for the former. Hence, this makes [Fe(miHpbmi)(2)](PF6)(4) a promising pH-insensitive analogue of [Fe(cpbmi)(2)](PF6)(2). Finally, the excited-state dynamics of the title compound [Fe(miHpbmi)(2)](PF6)(4) was investigated in solvents with different viscosities, however, showing very little dependency of the depopulation of the excited states on the properties of the solvent used.

This thesis explores the photophysics of some transition-metal complexes (TMCs) which utilize N-heterocyclic carbenes as ligands. After a historical interlude which traces the development of the broader field of transition metal complexes and their photophysical investigations, there is an overview of theoretical concepts and the spectroscopic methods employed. The focus thereafter is placed on complexes of the type [ML₂]ⁿ⁺ (where M=Fe and Mn) which feature the tripodal ‘Scorpionate’ motif, i.e. L=[phenyl(tris(3-methylimidazol-1-ylidene))borate]^–. L, like many carbenes, is an exceptional sigma-donor, and by some metrics is the strongest tripodal donor known. It is therefore able to sufficiently destabilize metal-centred states in conjunction with several 3d metals, allowing for the realization of long-lived charge-transfer states on the nanosecond timescale, in sharp contrast to many complexes based on polypyridyl ligand motifs previously investigated.

[Fe^IIIL₂]⁺ features a 2 ns doublet ligand-to-metal charge transfer (LMCT) excited state, which is substantially energetic and is shown to be capable of engaging in photoinduced electron transfer reactions with both donors and acceptors. The strong ligand field imposed on the iron centre furthermore makes possible the occurrence of two metal-centred redox events before the ligand oxidation – this translates to the unusual situation of the LMCT excited state of [Fe^IIIL₂]⁺ being able to oxidize or reduce its own ground state: a phenomenon called photoinduced symmetry-breaking charge separation. The finding is the first documented case with direct evidence for a transition-metal complex, and the only one which proceeds with a substantial driving force generally. [Mn^IVL₂]²⁺ features a long-lived LMCT excited state, which is found to be a potent photo-oxidant, capable of oxidizing a range of substrates including solvents such as methanol. Its excited state lifetime of 16 ns also presents a near order of magnitude improvement over the iron counterpart. One possible cause is traced to the spin-forbidden nature of the transition back to the ground state, highlighting the importance of such a design principle for the realization of longer lifetimes, as has been the case previously for excited states based on precious metals. The last half of the thesis features benzothiadiazole-Au-carbene (and phosphine) chromophores that are bright phosphors in room temperature solution – it is found that the carbene is inconsequential to the photophysics in this case, which is instead contingent on the direct linkage of the gold atom to a heteroarene moiety, causing an efficient population of its triplet manifold. Concluding remarks are furnished.