Léo Boivin, Élodie V. d’Astous, Adrien Schlachter, Daniel Fortin, Paul-Ludovic Karsenti, Christophe Lescop, Philippe Dauphin-Ducharme and Pierre D. Harvey
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Its X-ray structure reveals a series of piled 2D-layers separated by ∼3.55 Å, inside which π-stacked <strong>L</strong><small><sub>2</sub></small> pairs are placed in a head-to-tail conformation (interplanar <strong>L⋯L</strong> distance is ∼3.41 Å) and assembled by (C<img>N)<small><sub>2</sub></small><strong>Cu(μ-Br)2Cu</strong>(N<img>C)<small><sub>2</sub></small> rhomboids as secondary building units (SBUs) where each nitrile fragment links different <strong>L</strong>'s. <strong>UDS-6</strong> exhibits several interesting photonic properties such as a large absorption spectrum extending to ∼1700 nm, a near-infrared (NIR) and anti-Kasha emission (<em>λ</em><small><sub>em</sub></small> ∼ 1000 nm), exciton migration across the solid and photoconductivity, all of which drastically differ from those of <strong>L</strong> in the solid state (absorption extends to ∼600 nm, <em>λ</em><small><sub>em</sub></small> ∼ 700 nm, and <strong>L</strong> is not a photoconductor). Density functional theory (DFT) computations indicate that the lowest energy excited states are metal-halide-to-ligand charge transfer (MXLCT) states where the electron rich Cu<small><sub>2</sub></small>Br<small><sub>2</sub></small> units and the electron withdrawing <strong>L</strong> act as the electron density donor and acceptor, respectively. <strong>UDS-6</strong> is a photoconductor on its own and a mechanism study reveals the presence of photo-induced electron transfer (ET) in a 1 : 1 blend composed of tetraphenylporphyrinzinc(<small>II</small>), ZnTPP, a well-known electron donor, and <strong>L</strong> within the structure of <strong>UDS-6</strong> with a rate, <em>k</em><small><sub>ET</sub></small>, of 5.4 × 10<small><sup>7</sup></small> s<small><sup>−1</sup></small>, which assigns <strong>L</strong> as the electron acceptor and consequently the charge carrier in <strong>UDS-6</strong>.</p>","PeriodicalId":5,"journal":{"name":"ACS Applied Materials & Interfaces","volume":null,"pages":null},"PeriodicalIF":8.3000,"publicationDate":"2024-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"From a simple push–pull dye to a broad-band absorbing and photoconducting material by assembly with CuBr†\",\"authors\":\"Léo Boivin, Élodie V. d’Astous, Adrien Schlachter, Daniel Fortin, Paul-Ludovic Karsenti, Christophe Lescop, Philippe Dauphin-Ducharme and Pierre D. 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引用次数: 0
摘要
利用推拉发色团配体 2-(9H-亚芴基)丙二腈(L)和适度但非无毒的 CuBr 盐,我们设计出了一种热稳定和电化学稳定的二维配位聚合物(CP),其化学式为 [Cu2Br2L2]n(UDS-6)。它的 X 射线结构显示了一系列堆叠的二维层,层间相隔 ∼ 3.55 Å,层内的π堆叠 L2 对呈头尾构象(平面间 L⋯L 间距为 ∼ 3.41 Å),并由 (CN)2Cu(μ-Br)2Cu(NC)2 菱形体作为次级构建单元(SBU)组装而成,其中每个腈片段都连接着不同的 L。UDS-6 显示出几种有趣的光子特性,如延伸至 ∼1700 纳米的大吸收光谱、近红外(NIR)和反卡莎发射(λem ∼ 1000 纳米)、激子在固体中迁移以及光电导性,所有这些特性都与固态 L 的特性(吸收延伸至 ∼600 纳米,λem ∼ 700 纳米,且 L 不是光电导体)大不相同。密度泛函理论(DFT)计算表明,最低能量激发态是金属-卤化物-配体电荷转移(MXLCT)态,其中富电子的 Cu2Br2 单元和抽电子的 L 分别充当电子密度供体和受体。UDS-6 本身就是一种光电导体,其机理研究表明,在由四苯基苯并呋喃组成的 1 :光诱导电子转移(ET)是由四苯基卟啉锌(II)、ZnTPP(一种著名的电子供体)和 UDS-6 结构中的 L 组成的 1 : 1 混合体,其速率 kET 为 5.4 × 107 s-1,这表明 L 是电子受体,因此是 UDS-6 中的电荷载体。
From a simple push–pull dye to a broad-band absorbing and photoconducting material by assembly with CuBr†
A thermally and electrochemically stable 2D coordination polymer (CP) of formula [Cu2Br2L2]n (UDS-6) has been designed using the push–pull chromophore ligand 2-(9H-fluorenylidene)malononitrile (L) and the modest and yet non-innocent CuBr salt. Its X-ray structure reveals a series of piled 2D-layers separated by ∼3.55 Å, inside which π-stacked L2 pairs are placed in a head-to-tail conformation (interplanar L⋯L distance is ∼3.41 Å) and assembled by (CN)2Cu(μ-Br)2Cu(NC)2 rhomboids as secondary building units (SBUs) where each nitrile fragment links different L's. UDS-6 exhibits several interesting photonic properties such as a large absorption spectrum extending to ∼1700 nm, a near-infrared (NIR) and anti-Kasha emission (λem ∼ 1000 nm), exciton migration across the solid and photoconductivity, all of which drastically differ from those of L in the solid state (absorption extends to ∼600 nm, λem ∼ 700 nm, and L is not a photoconductor). Density functional theory (DFT) computations indicate that the lowest energy excited states are metal-halide-to-ligand charge transfer (MXLCT) states where the electron rich Cu2Br2 units and the electron withdrawing L act as the electron density donor and acceptor, respectively. UDS-6 is a photoconductor on its own and a mechanism study reveals the presence of photo-induced electron transfer (ET) in a 1 : 1 blend composed of tetraphenylporphyrinzinc(II), ZnTPP, a well-known electron donor, and L within the structure of UDS-6 with a rate, kET, of 5.4 × 107 s−1, which assigns L as the electron acceptor and consequently the charge carrier in UDS-6.
期刊介绍:
ACS Applied Materials & Interfaces is a leading interdisciplinary journal that brings together chemists, engineers, physicists, and biologists to explore the development and utilization of newly-discovered materials and interfacial processes for specific applications. Our journal has experienced remarkable growth since its establishment in 2009, both in terms of the number of articles published and the impact of the research showcased. We are proud to foster a truly global community, with the majority of published articles originating from outside the United States, reflecting the rapid growth of applied research worldwide.