钪
硼
结晶学
二次谐波产生
群(周期表)
晶体结构
非线性光学
多面体
离子
非线性光学
紫外线
Crystal(编程语言)
化学
材料科学
无机化学
非线性系统
光学
光电子学
物理
数学
有机化学
激光器
几何学
量子力学
程序设计语言
计算机科学
作者
Wenhao Liu,Xiaomeng Liu,Xianghe Meng,Chunxiao Li,Mengran Sun,Zheshuai Lin,Jiyong Yao
标识
DOI:10.1016/j.jallcom.2022.163832
摘要
• The non-centrosymmetric borates K 3 ScB 6 O 12 and K 6 NaSrSc 2 B 15 O 30 were found by spontaneous crystallization method. • Both K 3 ScB 6 O 12 and K 6 NaSrSc 2 B 15 O 30 exhibit wide band gaps of 5.75 and 5.92 eV, respectively. • K 6 NaSrSc 2 B 15 O 30 possesses type-I phase matching capability. • The SHG response in K 6 NaSrSc 2 B 15 O 30 is derived mainly from the [B 5 O 10 ] 5− groups and ScO 6 polyhedra. The spontaneous crystallization approach was used to synthesize two non-centrosymmetric scandium borate crystal materials, K 3 ScB 6 O 12 ( 1 ) and K 6 NaSrSc 2 B 15 O 30 ( 2 ), possessing the [B 5 O 10 ] 5− group. Both compounds exhibit wide band gaps of 5.75 and 5.92 eV, respectively. The second harmonic generation (SHG) effects of 1 and 2 are 1.3 and 0.7 times that of the commercial material KH 2 PO 4 (KDP), respectively. According to the Kurtz-Perry approach, 2 demonstrates type-I phase-matchable. First-principles calculations on 2 are done to better understand the link between structure and performance. The calculated results reveal that the discrete arrangement of [B 5 O 10 ] 5− groups and the distorted ScO 6 polyhedra in the structure are mainly responsible for the SHG response of 2 . Furthermore, since 1 and 2 possess short ultraviolet (UV) cut-off edges, they may be applicable as nonlinear optical (NLO) materials in the UV region.
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