LiPb <sub>3</sub> GeS <sub>4</sub> Cl <sub>3</sub> : Quasi‐T <sub>2</sub> ‐Supertetrahedral 3D Framework Enabling Superior Optical Performance

Y Yuhan Hu R Ruixi Wang (College of Chemistry Beijing Normal University Beijing 100875 P.R. China) S Shuang Zhao (Ministry of Education Key Laboratory of Cluster Science, Beijing Key Laboratory of Photoelectronic/Electrophotonic Conversion Materials, Frontiers Science Center for High Energy Materials, School of Chemistry and Chemical Engineering, Advanced Technology Research Institute (Jinan), Advanced Research Institute of Multidisciplinary Science) Y Yuzhuo Yang (Faculty of Arts and Sciences, Beijing Normal University , Zhuhai 519087,) J Jingyu Guo L Li‐Ming Wu (Center For Advanced Materials Research Beijing Normal University Zhuhai China) L Ling Chen (State Key Laboratory of Chemical Resource Engineering, College of Chemistry)

Abstract

Abstract The anisotropic structure building unit involving diverse chemical bond (ABUCB) has been proven effective in exploring high‐performance nonlinear optical (NLO) materials, through simultaneously enhancing second harmonic generation (SHG) and birefringence ( ∆n ). Building on this concept, we propose a strategy that employs different types of primary tetrahedra to construct anisotropic supertetrahedron (T 2 ). As a demonstration, we report a novel compound assembled by a quasi‐T 2 ‐supertetrahedron, LiPb 3 GeS 4 Cl 3 (LPGSC), exhibiting the superior optical properties among known thiogermanate halides and supertetrahedron‐chalcogenides. In the structure, there are two crystallographically independent Pb sites: Pb(1) forms the heterometallic T 2 ‐supertetrahedron [GePb(1) 3 S 8 ], while Pb(2) occupies an interstitial site with a labile coordination environment. As demonstrated by a series of samples Li x Pb 3.5‐ x /2 GeS 4 Cl 3 (L x PGSC, x  = 1‒0), the Pb(2) site can be substituted by lithium. Together with theoretical studies, we demonstrate that lithium incorporation effectively activates non‐bonding states (Pb‐6 s 2 , S‐3 p , Cl‐3 p ) near the Fermi level. This activation significantly enhances the second‐order NLO susceptibility (LPGSC: d 33  = 36.01 vs. AGS: d 36  = 18.67 pm V −1 ) and polarity anisotropy (LPGSC: ∆n cal. = 0.09 vs. AGS: 0.03 at 546 nm).

Article Details

Volume / Issue Vol. 65, Issue 2
Published January 09, 2026
ISSN 1433-7851
Publisher Wiley

Journal Info

Angewandte Chemie International Edition

Wiley

ISSN: 1433-7851 Physical Sciences

Authors (7)

Y

Yuhan Hu

R

Ruixi Wang

College of Chemistry Beijing Normal University Beijing 100875 P.R. China

S

Shuang Zhao

Ministry of Education Key Laboratory of Cluster Science, Beijing Key Laboratory of Photoelectronic/Electrophotonic Conversion Materials, Frontiers Science Center for High Energy Materials, School of Chemistry and Chemical Engineering, Advanced Technology Research Institute (Jinan), Advanced Research Institute of Multidisciplinary Science

Y

Yuzhuo Yang

Faculty of Arts and Sciences, Beijing Normal University , Zhuhai 519087,

J

Jingyu Guo

L

Li‐Ming Wu

Center For Advanced Materials Research Beijing Normal University Zhuhai China

L

Ling Chen

State Key Laboratory of Chemical Resource Engineering, College of Chemistry