journal article·2026-06-24

Achieving Excellent Nonlinear Optics in α ‑Ba 2 Ge 4 S 10 via Flux‑Induced Symmetry Breaking

Ying Guo, Guo‐Qiang Wang, Yan Guo, Xiao‐Ming Jiang, Bin‐Wen Liu, Guo‐Cong Guo

Publisher page

Abstract

ABSTRACT Although noncentrosymmetry is an essential prerequisite for second‐order nonlinear optical (NLO) effects, achieving it remains synthetically challenging. To date, the flux method has seldom been utilized to induce a transition from centrosymmetric to noncentrosymmetric structure. Herein, we successfully synthesized the noncentrosymmetric α ‐Ba 2 Ge 4 S 10 phase via flux‐induced symmetry breaking from centrosymmetric β ‐Ba 2 Ge 4 S 10 , enabling the growth of millimeter‐sized single crystal (up to 10 × 4 × 4 mm 3 ) using a sealed‐system flux method. Structurally, the structure of α ‐Ba 2 Ge 4 S 10 consists of zero‑dimensional supertetrahedral [Ge 4 S 10 ] 4– clusters charge‐balanced by Ba 2+ ions. Optically, α ‐Ba 2 Ge 4 S 10 displays a competitive phase‑matching second‐harmonic generation response (1.2 × AgGaS 2 @2050 nm) and a broad infrared transparency range (2.5–12.8 µm). To our knowledge, this is the first NLO material based on T2‐[Ge 4 S 10 ] clusters. Moreover, the introduction of electropositive Ba 2+ as a structural spacer in α ‐Ba 2 Ge 4 S 10 contributes to a wide optical band gap (3.15 eV) and a significantly enhanced laser‑induced damage threshold (14.8 × AgGaS 2 ), underscoring its promising NLO applicability. This study demonstrates that controlled phase transformation from centrosymmetric to noncentrosymmetric structures via the flux method offers a viable strategy for designing high‑performance NLO materials.
Source: crossref · Quality: baseline

Research context

OpenAlex topics: Crystal Structures and Properties · 2D Materials and Applications · Chalcogenide Semiconductor Thin Films

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

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

University of Chinese Academy of Sciences Beijing P. R. China

Materials Science and Engineering Fuzhou University Fuzhou Fujian P. R. China

Fujian Science&Technology Innovation Laboratory for Optoelectronic Information of China Fuzhou Fujian P. R. China

Funding

National Natural Science Foundation of China · Natural Science Foundation of Fujian Province · Youth Innovation Promotion Association of the Chinese Academy of Sciences

References (65)

Show source-provided references
1. 10.1038/s41586‐025‐10007‐z10.1038/s41586‐025‐10007‐z ↗
2. 10.1021/jacs.5b0792010.1021/jacs.5b07920 ↗
3. 10.1002/anie.20252006510.1002/anie.202520065 ↗
4. 10.1002/anie.20250923810.1002/anie.202509238 ↗
5. 10.1038/s41467‐024‐47209‐410.1038/s41467‐024‐47209‐4 ↗
6. 10.1002/anie.20242538410.1002/anie.202425384 ↗
7. 10.1002/anie.20231942410.1002/anie.202319424 ↗
8. 10.31635/ccschem.025.20250579910.31635/ccschem.025.202505799 ↗
9. 10.1021/acs.chemmater.5c0087010.1021/acs.chemmater.5c00870 ↗
10. 10.1002/anie.20252106610.1002/anie.202521066 ↗
11. 10.1002/anie.20252086110.1002/anie.202520861 ↗
12. 10.1021/acs.chemmater.4c0055110.1021/acs.chemmater.4c00551 ↗
13. 10.1039/d4dt01206b10.1039/d4dt01206b ↗
14. 10.1002/chem.20240073910.1002/chem.202400739 ↗
15. 10.1016/j.cjsc.2025.10070810.1016/j.cjsc.2025.100708 ↗
16. Nikogosyan D. N. · 2005
17. 10.1093/nsr/nwac01710.1093/nsr/nwac017 ↗
18. 10.1002/anie.20250225210.1002/anie.202502252 ↗
19. 10.1002/anie.20240631810.1002/anie.202406318 ↗
20. 10.1002/ange.20220161610.1002/ange.202201616 ↗
21. 10.1002/anie.20250087710.1002/anie.202500877 ↗
22. 10.1002/anie.20231564710.1002/anie.202315647 ↗
23. 10.1002/anie.20252609310.1002/anie.202526093 ↗
24. 10.1002/anie.20251036310.1002/anie.202510363 ↗
25. 10.1021/acs.cgd.2c0087710.1021/acs.cgd.2c00877 ↗
26. 10.1039/D4QI01781A10.1039/D4QI01781A ↗
27. 10.1039/d4sc01259c10.1039/d4sc01259c ↗
28. 10.1039/D0QI01071E10.1039/D0QI01071E ↗
29. 10.1002/advs.20220763010.1002/advs.202207630 ↗
30. 10.1021/acs.chemmater.4c0031010.1021/acs.chemmater.4c00310 ↗
31. 10.1002/anie.20200104210.1002/anie.202001042 ↗
32. 10.1002/anie.20250467310.1002/anie.202504673 ↗
33. 10.1002/anie.20250991710.1002/anie.202509917 ↗
34. 10.1002/anie.20211537410.1002/anie.202115374 ↗
35. 10.1021/ja909484610.1021/ja9094846 ↗
36. 10.1107/S056774088200640210.1107/S0567740882006402 ↗
37. 10.1016/j.jssc.2009.11.03010.1016/j.jssc.2009.11.030 ↗
38. 10.1016/S0022‐0248(02)01693‐710.1016/S0022‐0248(02)01693‐7 ↗
39. A New‐Type Ultraviolet SHG Crystal α‐BaB2O4
40. 10.1016/0022‐4596(73)90085‐610.1016/0022‐4596(73)90085‐6 ↗
41. 10.1021/acs.inorgchem.1c0114910.1021/acs.inorgchem.1c01149 ↗
42. 10.1021/acs.inorgchem.8b0123810.1021/acs.inorgchem.8b01238 ↗
43. 10.1021/acs.inorgchem.8b0143710.1021/acs.inorgchem.8b01437 ↗
44. 10.1016/j.jssc.2021.12222610.1016/j.jssc.2021.122226 ↗
45. 10.1007/s10853‐017‐1215‐210.1007/s10853‐017‐1215‐2 ↗
46. 10.1107/S010876810601322X10.1107/S010876810601322X ↗
47. 10.1039/d2qi01263d10.1039/d2qi01263d ↗
48. 10.1021/acs.jpclett.8b0289210.1021/acs.jpclett.8b02892 ↗
49. 10.1002/pssa.221013011610.1002/pssa.2210130116 ↗
50. 10.1039/D1QI00879J10.1039/D1QI00879J ↗
51. 10.1039/D2QI00937D10.1039/D2QI00937D ↗
52. 10.1039/D2MH01200F10.1039/D2MH01200F ↗
53. 10.1021/acs.chemmater.0c0300810.1021/acs.chemmater.0c03008 ↗
54. 10.1103/PhysRevB.79.24520310.1103/PhysRevB.79.245203 ↗
55. 10.1063/1.165685710.1063/1.1656857 ↗
56. 10.1016/j.jallcom.2019.04.32110.1016/j.jallcom.2019.04.321 ↗
57. 10.1016/j.jallcom.2019.04.32110.1016/j.jallcom.2019.04.321 ↗
58. 10.1021/acs.cgd.7b0158610.1021/acs.cgd.7b01586 ↗
59. 10.1021/jacs.0c0473810.1021/jacs.0c04738 ↗
60. 10.1039/D0TC05952H10.1039/D0TC05952H ↗
61. 10.1039/C3TC31872A10.1039/C3TC31872A ↗
62. 10.1021/acsami.3c1552910.1021/acsami.3c15529 ↗
63. Perturbation Expansion of Variational Principles at Arbitrary Order10.1103/PhysRevA.52.1086 ↗
64. 10.1021/acsami.4c2247210.1021/acsami.4c22472 ↗
65. 10.1002/anie.20191241610.1002/anie.201912416 ↗