Spiral transition-metal dichalcogenides with broken crystal inversion symmetry and significant second-order nonlinear responses have shown great promise for further nonlinear optical applications. However, various spiral structures will be formed during their synthesis process, their second harmonic generation (SHG) varying with the layer thickness and which of them manifesting the most promising SHG response are still unresolved. Here, the layer-dependent SHG response is investigated for four representative spiral WS with different screw and twist angles, including aligned- and twisted-triangular spiral structures, aligned- and twisted-hexagonal spiral structures, respectively. Experimental results demonstrate that both aligned- and twisted-hexagonal spiral WS present weak SHG response. In contrast, the SHG signal of the aligned-triangular spiral WS almost quadratically increases with the lift of their thickness, which is two orders of magnitude stronger than hexagonal structures. Moreover, an oscillating layer-dependence SHG response for twisted-triangular spiral WS has been attributed to the restored inversion symmetry. The underlying mechanism has been explored by the evolution of their crystal symmetry. The results not only disclose that the nonlinear response of the spiral WS can be tailored on-demand through the novel structural designs, but also pave the way to scalable integrated photonics and lab-on-a-chip quantum devices based on spiral layered materials.
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http://dx.doi.org/10.1002/adma.202415214 | DOI Listing |
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March 2025
School of Chemistry and Chemical Engineering, Yangzhou University, 180 Siwangting Road, Yangzhou, 250002, China.
The pressing demand for both established and innovative technologies to expand laser wavelengths has rendered high-performance nonlinear optical (NLO) crystals with large optical anisotropy indispensable. Here, centrosymmetric [SHC(NH)]CdBr (1) and pseudo-2D layered [SC(NH)]CdBr (2), as well as pseudo-3D noncentrosymmetric [SC(NH)]CdCl (3) are successfully synthesized through the introduction of π-conjugated SC(NH) groups. Compared to ionic compound 1 containing full-halogen coordination tetrahedra, covalent compounds 2 and 3 featuring novel polar [SC(NH)]CdX (X = Br, Cl) tetrahedral units demonstrate enhanced bandgaps (>4 eV) and birefringences (>0.
View Article and Find Full Text PDFPhys Chem Chem Phys
March 2025
Department of Chemistry, Faculty of Science, The M.S. University of Baroda, Vadodara-390002, Gujarat, India.
When aqueous solutions of KSCN and Hg(CN) were mixed, we observed the formation of long, needle-shaped single crystals with an unexpected structure and a formula of KHg(CN)(SCN). Single-crystal X-ray diffraction revealed that the CN ligands remain confined to the two apical positions of Hg(II) without forming an extended network. Instead, the sulphur atoms create a layered structure by forming four S-Hg bonds (3.
View Article and Find Full Text PDFAngew Chem Int Ed Engl
March 2025
State Key Laboratory of Crystal Materials and Institute of Crystal Materials, Shandong University, Jinan, 250100, China.
The contradictory relationship between band gaps and the second-harmonic generation (SHG) response constitutes a formidable challenge in the rational design of infrared nonlinear optical (IR NLO) crystals. In oxide-based crystals, the incorporation of strongly distorted octahedra containing d° cations as central elements are a common approach to enhance SHG responses, while inadvertently leading to a significant decrease in band gaps due to the unfavorable energy level splitting. In this study, an innovative "4d/5s electron band-inversion" strategy is introduced to enhance SHG response while preserving a wide band gap within the octahedron-symmetry-protected langasite structure.
View Article and Find Full Text PDFInorg Chem
March 2025
College of Chemistry, Sichuan University, Chengdu 610064, China.
Using chiral amino acids as terminal ligands, colorless crystals of Cd(SCN)(l-CHNO)(HO)·0.5CHOH () and Cd(SCN)(l-CHNO) () were obtained by a solvent evaporation method. Compound has a layered structure with a moderate second harmonic generation (SHG) efficiency (0.
View Article and Find Full Text PDFAngew Chem Int Ed Engl
March 2025
Tianjin Key Laboratory of Functional Crystal Materials, Institute of Functional Crystal, College of Materials Science and Engineering, Tianjin University of Technology, Tianjin, 300384, China.
Deep-ultraviolet nonlinear optical (DUV NLO) crystals play a vitally important role in many scientific and technological fields, yet their rational design remains an ongoing challenge. Here, through utilizing the ordered structure design, a new KBeBOF-like DUV transparent NLO crystal CsKY(BO) has been successfully designed and synthesized, in which we first use the largest π-conjugated BO functional groups to substitute the BO to maximize the second-harmonic generation (SHG) response and utilize the K/YO connecting groups to replace two BeOF groups to optimize the layer connections. Eventually, CsKY(BO) exhibits not only the largest SHG responses in KBeBOF-like DUV borates but also the best growth rate along c axis (the strong layer-habit along c axis has been being the greatest obstacle to prohibit the practical application of KBeBOF and its derivative).
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