Interlayer Electronic Decoupling Unlocks Giant Birefringence in π‐Conjugated Metal‐Organic Frameworks

J Jia‐Xiang Zhang (State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou 350002 P.R. China) X Xinyan Wu W Weishan Li (National Key Laboratory of Advanced Micro and Nano Manufacture Technology, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, School of Materials Science and Engineering) H Haolin Zhong (National Key Laboratory of Advanced Micro and Nano Manufacture Technology School of Materials Science and Engineering Peking University Beijing China) J Jinkun Guo (National Key Laboratory of Advanced Micro and Nano Manufacture Technology, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, School of Materials Science and Engineering) Q Qingsheng Zeng M Mao‐Yin Ran (Yunnan Key Laboratory of Electromagnetic Materials and Devices School of Materials and Energy Yunnan University Kunming China) Z Ze‐Fan Yao (Beijing National Laboratory For Molecular Sciences (BNLMS) Key Laboratory of Polymer Chemistry and Physics of Ministry of Education Center For Soft Matter Science and Engineering College of Chemistry and Molecular Engineering Peking University Beijing China) Y Yu‐Qing Zheng (National Key Laboratory of Advanced Micro and Nano Manufacture Technology Beijing Advanced Innovation Center for Integrated Circuits School of Integrated Circuits Peking University Beijing China) Q Qingqing Ji (School of Physical Science and Technology) J Jin‐Hu Dou (National Key Laboratory of Advanced Micro and Nano Manufacture Technology Key Laboratory of Polymer Chemistry and Physics of Ministry of Education School of Materials Science and Engineering Peking University Beijing 100871 P.R. China)

Abstract

ABSTRACT Giant birefringence (Δ n > 1.0) is an essential requirement and a remaining challenge for advanced polarization optics. Organic π‐conjugated molecules possess high intrinsic polarizability favorable for birefringent materials design, although this potential is often hindered by dense, cofacial π–π stacking, which induces strong interlayer electronic coupling and severely limits optical anisotropy. Metal‐organic frameworks (MOFs) offer a solution that utilizes coordination bonds to modulate the packing configuration of ligands. However, a dimensionality dilemma remains: 3D MOFs often possess high symmetry that cancels optical anisotropy, while 2D MOFs typically inherit eclipsed stacking of conjugated ligands, locking birefringence at low levels. Herein, we propose an anion‐induced coordination competition strategy (AICCS) to disrupt dense stacking. By steering inorganic anions ( T d of SO 4 2− and D 3h of NO 3 − ) and π‐conjugated 2,3,6,7,10,11‐hexahydroxytriphenylene (HHTP) ligands to competitively coordinate with La 3+ , we successfully force in‐plane slip of adjacent HHTP layers in resulted MOFs. This precisely engineered slip‐stacking decouples interlayer electronic states and liberates the latent polarizability of the π‐system. Consequently, we achieved a dramatic birefringence enhancement from the suppressed state in the parent LaHHTP (Δ n = 0.12) to record‐high values of Δ n = 1.1 in LaHHTP‐SO 4 and Δ n = 1.3 in LaHHTP‐NO 3 , providing a versatile route to design next‐generation anisotropic optical crystals.

Article Details

Volume / Issue Vol. 1, Issue 1
Published June 18, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (11)

J

Jia‐Xiang Zhang

State Key Laboratory of Structural Chemistry Fujian Institute of Research on the Structure of Matter Chinese Academy of Sciences Fuzhou 350002 P.R. China

X

Xinyan Wu

W

Weishan Li

National Key Laboratory of Advanced Micro and Nano Manufacture Technology, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, School of Materials Science and Engineering

H

Haolin Zhong

National Key Laboratory of Advanced Micro and Nano Manufacture Technology School of Materials Science and Engineering Peking University Beijing China

J

Jinkun Guo

National Key Laboratory of Advanced Micro and Nano Manufacture Technology, Key Laboratory of Polymer Chemistry and Physics of Ministry of Education, School of Materials Science and Engineering

Q

Qingsheng Zeng

M

Mao‐Yin Ran

Yunnan Key Laboratory of Electromagnetic Materials and Devices School of Materials and Energy Yunnan University Kunming China

Z

Ze‐Fan Yao

Beijing National Laboratory For Molecular Sciences (BNLMS) Key Laboratory of Polymer Chemistry and Physics of Ministry of Education Center For Soft Matter Science and Engineering College of Chemistry and Molecular Engineering Peking University Beijing China

Y

Yu‐Qing Zheng

National Key Laboratory of Advanced Micro and Nano Manufacture Technology Beijing Advanced Innovation Center for Integrated Circuits School of Integrated Circuits Peking University Beijing China

Q

Qingqing Ji

School of Physical Science and Technology

J

Jin‐Hu Dou

National Key Laboratory of Advanced Micro and Nano Manufacture Technology Key Laboratory of Polymer Chemistry and Physics of Ministry of Education School of Materials Science and Engineering Peking University Beijing 100871 P.R. China