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Strategies for Design of Potential Singlet Fission Chromophores Utilizing a Combination of Ground-State and Excited-State Aromaticity Rules

[Image: see text] Singlet exciton fission photovoltaic technology requires chromophores with their lowest excited states arranged so that 2E(T(1)) < E(S(1)) and E(S(1)) < E(T(2)). Herein, qualitative theory and quantum chemical calculations are used to develop explicit strategies on how to use...

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Detalles Bibliográficos
Autores principales: El Bakouri, Ouissam, Smith, Joshua R., Ottosson, Henrik
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7307911/
https://www.ncbi.nlm.nih.gov/pubmed/32107921
http://dx.doi.org/10.1021/jacs.9b12435
Descripción
Sumario:[Image: see text] Singlet exciton fission photovoltaic technology requires chromophores with their lowest excited states arranged so that 2E(T(1)) < E(S(1)) and E(S(1)) < E(T(2)). Herein, qualitative theory and quantum chemical calculations are used to develop explicit strategies on how to use Baird’s 4n rule on excited-state aromaticity, combined with Hückel’s 4n + 2 rule for ground-state aromaticity, to tailor new potential chromophores for singlet fission. We first analyze the E(T(1)), E(S(1)), and E(T(2)) of benzene and cyclobutadiene (CBD) as excited-state antiaromatic and aromatic archetypes, respectively, and reveal that CBD fulfills the criteria on the state ordering for a singlet fission chromophore. We then look at fulvenes, a class of compounds that can be tuned by choice of substituents from Baird-antiaromatic to Baird-aromatic in T(1) and S(1) and from Hückel-aromatic to Hückel-antiaromatic in S(0). The T(1) and S(1) states of most substituted fulvenes (159 of 225) are described by singly excited HOMO → LUMO configurations, providing a rational for the simultaneous tuning of E(T(1)) and E(S(1)) along an approximate (anti)aromaticity coordinate. Key to the tunability is the exchange integral (K(H,L)), which ideally is constant throughout the compound class, providing a constant ΔE(S(1) – T(1)). This leads us to a geometric model for the identification of singlet fission chromophores, and we explore what factors limit the model. Candidates with calculated E(T(1)) values of ∼1 eV or higher are identified among benzannelated 4nπ-electron compound classes and siloles. In brief, it is clarified how the joint utilization of Baird’s 4n and Hückel’s 4n + 2 rules, together with substituent effects (electronic and steric) and benzannelation, can be used to tailor new chromophores with potential use in singlet fission photovoltaics.