Topological Engineering From Non‐Emissive Chiral Metallomacrocycle to Interlocked Architecture for Strong Circularly Polarized Luminescence

J Jing‐Hao Wei (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China) L Lin‐Xi Shi (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China) X Xu‐Yang Ding (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China) B Bo‐Wen Dai (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China) J Jin‐Yun Wang (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China) F Feng‐Rong Dai (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China) H Han Cheng (State Key Laboratory of Precision and Intelligent Chemistry, School of Chemistry and Materials Science) Z Zhong‐Ning Chen (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China)

Abstract

ABSTRACT Interlocked architectures are crucial for stabilizing specific conformations to achieve superior performance. Herein, we proposes a vacant π‐site recombination strategy to achieve significant luminescence enhancement through topological engineering from non‐emissive chiral metallomacrocycles ( R / S ‐Au 4 ) to highly circularly polarized luminescence (CPL) catenanes ( R / S ‐Au 8 ). The dynamical structural transformation of metallomacrocycles ( R / S ‐Au 4 ) to catenanes ( R / S ‐Au 8 ) was monitored by 1 H and 31 P NMR spectroscopy. Excited state dynamics and theoretical studies revealed that the increase of heavy atom effect in catenanes ( R / S ‐Au 8 ) effectively increases spin‐orbit coupling constant from 4.03 ( R ‐Au 4 ) to 48.22 cm −1 ( R ‐Au 8 ), facilitating the intersystem crossing between S 1 and T 1 . While R / S ‐Au 4 with flexible metallocyclic structures tend to rapidly relax the excited states through thermally vibrational processes, interlocked structures of R / S ‐Au 8 lead to better rigidity, thus effectively suppressing non‐radiative deactivation and facilitating radiative T 1 →S 0 relaxation, thus achieving highly efficient CPL with ca. 39% quantum yield in solution. Solution‐processed circularly polarized organic light‐emitting diodes (CP‐OLEDs) based on R / S ‐Au 8 attain high‐efficiency deep‐red circularly polarized electroluminescence (CPEL) peaked at 685 nm, with external quantum efficiency (EQE) of 9.9% and electroluminescence asymmetric factor of ± 2.2 × 10 −3 . In any case, this upgrading approach from discrete macrocycles to interlocked architectures opens a new avenue for developing high‐performance emitting materials and devices.

Article Details

Volume / Issue Vol. 65, Issue 24
Published June 08, 2026
ISSN 1433-7851
Publisher Wiley

Journal Info

Angewandte Chemie International Edition

Wiley

ISSN: 1433-7851 Physical Sciences

Authors (8)

J

Jing‐Hao Wei

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China

L

Lin‐Xi Shi

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China

X

Xu‐Yang Ding

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China

B

Bo‐Wen Dai

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China

J

Jin‐Yun Wang

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China

F

Feng‐Rong Dai

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China

H

Han Cheng

State Key Laboratory of Precision and Intelligent Chemistry, School of Chemistry and Materials Science

Z

Zhong‐Ning Chen

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou China