Multi‐Resonance Deep‐Red Emitters with Shallow Potential‐Energy Surfaces to Surpass Energy‐Gap Law

Efficient organic emitters in the deep‐red region are rare due to the “energy gap law”. Herein, multiple boron (B)‐ and nitrogen (N)‐atoms embedded polycyclic heteroaromatics featuring hybridized π‐bonding/ non‐bonding molecular orbitals are constructed, providing a way to overcome the above lumines...

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Veröffentlicht in:Angewandte Chemie International Edition 2021-09, Vol.60 (37), p.20498-20503
Hauptverfasser: Zhang, Yuewei, Zhang, Dongdong, Huang, Tianyu, Gillett, Alexander J., Liu, Yang, Hu, Deping, Cui, Linsong, Bin, Zhengyang, Li, Guomeng, Wei, Jinbei, Duan, Lian
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container_end_page 20503
container_issue 37
container_start_page 20498
container_title Angewandte Chemie International Edition
container_volume 60
creator Zhang, Yuewei
Zhang, Dongdong
Huang, Tianyu
Gillett, Alexander J.
Liu, Yang
Hu, Deping
Cui, Linsong
Bin, Zhengyang
Li, Guomeng
Wei, Jinbei
Duan, Lian
description Efficient organic emitters in the deep‐red region are rare due to the “energy gap law”. Herein, multiple boron (B)‐ and nitrogen (N)‐atoms embedded polycyclic heteroaromatics featuring hybridized π‐bonding/ non‐bonding molecular orbitals are constructed, providing a way to overcome the above luminescent boundary. The introduction of B‐phenyl‐B and N‐phenyl‐N structures enhances the electronic coupling of those para‐positioned atoms, forming restricted π‐bonds on the phenyl‐core for delocalized excited states and thus a narrow energy gap. The mutually ortho‐positioned B‐ and N‐atoms also induce a multi‐resonance effect on the peripheral skeleton for the non‐bonding orbitals, creating shallow potential energy surfaces to eliminate the high‐frequency vibrational quenching. The corresponding deep‐red emitters with peaks at 662 and 692 nm exhibit narrow full‐width at half‐maximums of 38 nm, high radiative decay rates of ca. 108 s−1, ≈100 % photo‐luminescence quantum yields and record‐high maximum external quantum efficiencies of ca. 28 % in a normal planar organic light‐emitting diode structure, simultaneously. Polycyclic heteroaromatics containing multiple embedded boron (B)‐ and nitrogen (N)‐atoms and featuring hybridized π‐bonding/ non‐bonding molecular orbitals are constructed. They have enhanced electronic coupling for deep‐red emission almost reaching the red‐corner of CIE coordinates diagram and an induced multiple resonance (MR) effect to create a shallow potential energy surface, fundamentally overcoming the energy gap law.
doi_str_mv 10.1002/anie.202107848
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Herein, multiple boron (B)‐ and nitrogen (N)‐atoms embedded polycyclic heteroaromatics featuring hybridized π‐bonding/ non‐bonding molecular orbitals are constructed, providing a way to overcome the above luminescent boundary. The introduction of B‐phenyl‐B and N‐phenyl‐N structures enhances the electronic coupling of those para‐positioned atoms, forming restricted π‐bonds on the phenyl‐core for delocalized excited states and thus a narrow energy gap. The mutually ortho‐positioned B‐ and N‐atoms also induce a multi‐resonance effect on the peripheral skeleton for the non‐bonding orbitals, creating shallow potential energy surfaces to eliminate the high‐frequency vibrational quenching. The corresponding deep‐red emitters with peaks at 662 and 692 nm exhibit narrow full‐width at half‐maximums of 38 nm, high radiative decay rates of ca. 108 s−1, ≈100 % photo‐luminescence quantum yields and record‐high maximum external quantum efficiencies of ca. 28 % in a normal planar organic light‐emitting diode structure, simultaneously. Polycyclic heteroaromatics containing multiple embedded boron (B)‐ and nitrogen (N)‐atoms and featuring hybridized π‐bonding/ non‐bonding molecular orbitals are constructed. 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Herein, multiple boron (B)‐ and nitrogen (N)‐atoms embedded polycyclic heteroaromatics featuring hybridized π‐bonding/ non‐bonding molecular orbitals are constructed, providing a way to overcome the above luminescent boundary. The introduction of B‐phenyl‐B and N‐phenyl‐N structures enhances the electronic coupling of those para‐positioned atoms, forming restricted π‐bonds on the phenyl‐core for delocalized excited states and thus a narrow energy gap. The mutually ortho‐positioned B‐ and N‐atoms also induce a multi‐resonance effect on the peripheral skeleton for the non‐bonding orbitals, creating shallow potential energy surfaces to eliminate the high‐frequency vibrational quenching. The corresponding deep‐red emitters with peaks at 662 and 692 nm exhibit narrow full‐width at half‐maximums of 38 nm, high radiative decay rates of ca. 108 s−1, ≈100 % photo‐luminescence quantum yields and record‐high maximum external quantum efficiencies of ca. 28 % in a normal planar organic light‐emitting diode structure, simultaneously. Polycyclic heteroaromatics containing multiple embedded boron (B)‐ and nitrogen (N)‐atoms and featuring hybridized π‐bonding/ non‐bonding molecular orbitals are constructed. They have enhanced electronic coupling for deep‐red emission almost reaching the red‐corner of CIE coordinates diagram and an induced multiple resonance (MR) effect to create a shallow potential energy surface, fundamentally overcoming the energy gap law.</abstract><cop>WEINHEIM</cop><pub>Wiley</pub><pmid>34319641</pmid><doi>10.1002/anie.202107848</doi><tpages>6</tpages><edition>International ed. in English</edition><orcidid>https://orcid.org/0000-0003-2750-0972</orcidid><orcidid>https://orcid.org/0000-0001-6577-3432</orcidid><orcidid>https://orcid.org/0000-0002-7127-1102</orcidid><orcidid>https://orcid.org/0000-0002-6664-527X</orcidid><orcidid>https://orcid.org/0000-0001-7161-1253</orcidid></addata></record>
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subjects Boron
Chemical bonds
Chemistry
Chemistry, Multidisciplinary
Coupling (molecular)
Decay rate
Emitters
Energy
Energy gap
energy gap law
hybridized π-bonding/ non-bonding orbitals
Molecular orbitals
Nitrogen
OLEDs
Physical Sciences
polycyclic heteroaromatics
Potential energy
Resonance
Science & Technology
shallow potential energy surfaces
title Multi‐Resonance Deep‐Red Emitters with Shallow Potential‐Energy Surfaces to Surpass Energy‐Gap Law
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