Journal of the American Chemical Society · 2024 · 75 citations · 64 references
Natural SciencesMaterials SciencePhysicsElectronic MaterialsOptical MaterialsPhotonicsInfrared Optical MaterialsOptoelectronic DevicesOptoelectronic MaterialsOrganic Electronic MaterialsOrganic SemiconductorsPhotodetectorsActive MaterialsEmission SpectraIntermolecular Electron TransferOptoelectronic PropertiesOrganic PhotodetectorsPhotodetectionPhotodetector MaterialsRadiative Transitions
Organic molecules have been regarded as ideal candidates for near-infrared (NIR) optoelectronic active materials due to their customizability and ease of large-scale production. However, constrained by the intricate molecular design and severe energy gap law, the realization of optoelectronic devices in the second near-infrared (NIR (II)) region with required narrow band gaps presents more challenges. Herein, we have originally proposed a cocrystal strategy that utilizes intermolecular charge–transfer interaction to drive the redshift of absorption and emission spectra of a series BF X TQ ( X = 0, 1, 2, 4) cocrystals, resulting in the spectra located at NIR (II) window and reducing the optical bandgap to ∼0.98 eV. Significantly, these BF X TQ-based optoelectronic devices can exhibit dual-mode optoelectronic characteristics. An investigation of a series of BF X TQ-based photodetectors exhibits detectivity ( D *) surpassing 10 13 Jones at 375 to 1064 nm with a maximum of 1.76 × 10 14 Jones at 1064 nm. Moreover, the radiative transition of CT excitons within the cocrystals triggers NIR emission over 1000 nm with a photoluminescence quantum yield (PLQY) of ∼4.6% as well as optical waveguide behavior with a low optical-loss coefficient of 0.0097 dB/μm at 950 nm. These results promote the advancement of an emerging cocrystal approach in micro/nanoscale NIR multifunctional optoelectronics.
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