4.8 Article

Manipulating the Charge Transfer Absorption for Narrowband Light Detection in the Near-Infrared

期刊

CHEMISTRY OF MATERIALS
卷 31, 期 22, 页码 9325-9330

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acs.chemmater.9b02700

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资金

  1. UKRI EPSRC Doctoral Training Account studentship
  2. Welsh Government's Ser Cymru II Sustainable Advanced Materials Program (European Regional Development Fund)
  3. Welsh Government's Ser Cymru II Sustainable Advanced Materials Program (Welsh European Funding Office)
  4. Welsh Government's Ser Cymru II Sustainable Advanced Materials Program (Swansea University Strategic Initiative)
  5. German Federal Ministry for Education and Research (BMBF) through the InnoProfile project Organische p-i-n Bauelemente 2.2 [03IPT602X]
  6. Ser Cymru II Program Sustainable Advanced Materials (Welsh European Funding Office European Regional Development Fund)
  7. EPSRC [EP/N020863/1, 2105065] Funding Source: UKRI

向作者/读者索取更多资源

Charge generation and recombination processes at interfaces between electron donating (donor, D) and accepting molecules (acceptor, A) are mediated by intermolecular charge-transfer (CT) states. Since organic photovoltaic and photodetecting devices rely on D-A interfaces, an understanding of the molecular and morphological aspects governing CT state properties is crucial. In this paper, we synthesize a novel series of bi(thio)pyranylidene donor molecules and show how the interplay of molecular structure and energy levels in a D-C-60 blend affect the line shape of the CT absorption cross section. By rationally designing the molecule 2,2',6,6'-tetra-(2-methylthienyl)-4,4'-bithiopyranylidene, we achieve a 2 times stronger CT absorption peak than the literature-known molecule 2,2',6,6'-tetraphenyl-4,4'-bipyranylidene when blended with C-60. The low CT state energy combined with relatively strong CT absorption of this new material blend is exploited by fabricating near-infrared, cavity enhanced narrowband detectors. The photodetectors cover an impressive wavelength range from 810 to 1665 nm with line widths between 30 and 50 nm.

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