材料科学
双折射
硒
非线性光学
二次谐波产生
带隙
光学材料
非线性光学
折射率
光电子学
分析化学(期刊)
光学
非线性系统
激光器
有机化学
物理
化学
量子力学
冶金
作者
Pengfei Li,Ya‐Ping Gong,Chun‐Li Hu,Bo Zhang,Jiang‐Gao Mao,Fang Kong
标识
DOI:10.1002/adom.202301426
摘要
Abstract UV nonlinear optical materials require the simultaneous achievement of a large second harmonic generation (SHG) coefficient (≥1 × KH 2 PO 4 (KDP), d ij > 0.39 pmV −1 ), wide bandgap ( λ < 300 nm, E g > 4.2 eV), and moderate birefringence (0.05‐0.10@1064 nm) in a single structure. Therefore, designing UV nonlinear optical materials with excellent comprehensive performance is a challenging task. Herein, four UV transparent selenite materials are successfully obtained, namely, Al 2 (SeO 3 ) 3 (H 2 O) 3 (1), Ga 2 (SeO 3 ) 3 (H 2 O) 3 (2), NaGa 3 (HSeO 3 ) 6 (SeO 3 ) 2 (3), and Cd 5 Ga 4 (HSeO 3 ) 2 (SeO 3 ) 10 (4), through rational design and screening in the pure selenite system. Al 2 (SeO 3 ) 3 (H 2 O) 3 (1) and Ga 2 (SeO 3 ) 3 (H 2 O) 3 (2) are UV nonlinear optical materials with balanced properties, exhibiting moderate SHG responses (1.2 and 1.1 × KDP), appropriate birefringence (0.084 and 0.076@1064 nm), and wide bandgaps (5.5 and 5.3 eV). Such bandgaps are the largest in the reported pure selenite nonlinear optical (NLO) materials. This work further demonstrates that pure selenite is a good candidate for UV NLO materials.
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