2021
DOI: 10.1039/d0mh02032j
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Mechanically induced single-molecule white-light emission of excited-state intramolecular proton transfer (ESIPT) materials

Abstract: Described herein is the first example of mechanically induced single-molecule white-light emission based on excited-state intramolecular proton transfer (ESIPT) materials. Mechanism of mechanochromism is clearly disclosed by powder and single...

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Cited by 38 publications
(22 citation statements)
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“…14,15 Due to the presence of two excitedstate electronic configurations, the ESIPT molecules generally exhibit largely Stokes-shifted T* fluorescence or even dual fluorescence from both N* and T* states. 16,17 Modulating the ESIPT reaction for anticipant applications has been fascinating for material chemists. For instance, some near-infrared fluorescent materials are designed based on the occurrence of a highly exergonic ultrafast ESIPT reaction, 16,18,19 while some single-component white-light materials cover the entire visible region on account of the dual fluorescence originating from an ESIPT thermodynamic equilibrium, 17,20 and some deep-blue fluorescent materials are fabricated through prohibiting an undesired ESIPT reaction despite the preformation of intramolecular hydrogen bonds (intra-HB).…”
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confidence: 99%
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“…14,15 Due to the presence of two excitedstate electronic configurations, the ESIPT molecules generally exhibit largely Stokes-shifted T* fluorescence or even dual fluorescence from both N* and T* states. 16,17 Modulating the ESIPT reaction for anticipant applications has been fascinating for material chemists. For instance, some near-infrared fluorescent materials are designed based on the occurrence of a highly exergonic ultrafast ESIPT reaction, 16,18,19 while some single-component white-light materials cover the entire visible region on account of the dual fluorescence originating from an ESIPT thermodynamic equilibrium, 17,20 and some deep-blue fluorescent materials are fabricated through prohibiting an undesired ESIPT reaction despite the preformation of intramolecular hydrogen bonds (intra-HB).…”
mentioning
confidence: 99%
“…16,17 Modulating the ESIPT reaction for anticipant applications has been fascinating for material chemists. For instance, some near-infrared fluorescent materials are designed based on the occurrence of a highly exergonic ultrafast ESIPT reaction, 16,18,19 while some single-component white-light materials cover the entire visible region on account of the dual fluorescence originating from an ESIPT thermodynamic equilibrium, 17,20 and some deep-blue fluorescent materials are fabricated through prohibiting an undesired ESIPT reaction despite the preformation of intramolecular hydrogen bonds (intra-HB). 21 The strategies of modulating an ESIPT reaction could be mainly divided into extrinsic disturbance and intrinsic modification.…”
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confidence: 99%
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“…According to the colorimetric characteristics, white luminescence relies on a combination of blue, green, and red or blue and orange, covering the visible spectrum from 400 to 700 nm. Compared to multicomponent materials, white-light-emitting single molecules have the advantages of highly stable and repeatable spectra and the simple reproducible preparation of devices . There are various mechanisms for white-light emission, including excited-state intramolecular proton transfer (ESIPT), monomer and excimer fluorescence, intramolecular energy transfer (IET), charge transfer (CT), thermally activated delayed fluorescence (TADF), and fluorescence and phosphorescence dual emission. ESIPT luminescence involves two molecules with different forms, normal (N) and tautomeric (T) forms, which have an intramolecular hydrogen bond, a large Stokes shift, and no self-absorption. The proton donor (−OH or −NH 2 ) and the proton acceptor (N– or −CO) groups are in the proximity of each other with an intramolecular hydrogen bond in the five- or six-membered ring. , The ESIPT process starts with a molecule (N) on the electronic ground state and goes to excited states (N*), producing a tautomeric species T* through electronic density rearrangement, providing dual emission from two excited states [N* (S 1 ) → N (S 0 ) and T* (S 1 ) → T (S 0 )].…”
Section: Introductionmentioning
confidence: 99%