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LiMg(IO):一种通过单位点异价取代设计的优异二次谐波产生材料。

LiMg(IO): an excellent SHG material designed by single-site aliovalent substitution.

作者信息

Chen Jin, Hu Chun-Li, Mao Fei-Fei, Zhang Xiao-Han, Yang Bing-Ping, Mao Jiang-Gao

机构信息

State Key Laboratory of Structural Chemistry , Fujian Institute of Research on the Structure of Matter , Chinese Academy of Sciences , Fuzhou 350002 , P. R. China . Email:

University of Chinese Academy of Sciences , Beijing 100039 , P. R. China.

出版信息

Chem Sci. 2019 Oct 15;10(47):10870-10875. doi: 10.1039/c9sc04832d. eCollection 2019 Dec 21.

DOI:10.1039/c9sc04832d
PMID:32190241
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7066663/
Abstract

An excellent second harmonic generation (SHG) material, LiMg(IO) (LMIO), has been elaborately designed from LiM(IO) (M = Ti, Sn, and Ge) by aliovalent substitution of the central M cation followed by Wyckoff position exchange. The new structure sustains the ideal-alignment of (IO) groups. Importantly, LMIO exhibits an extremely strong SHG effect of roughly 24 × KHPO (KDP) under 1064 nm laser radiation or 1.5 × AgGaS (AGS) under 2.05 μm laser radiation, which is larger than that of α-LiIO (18 × KDP). The replacement of M with Mg without d-d electronic transitions induces an obviously larger band gap (4.34 eV) with a short absorption edge (285 nm). This study shows that single-site aliovalent substitution provides a new synthetic route for designing SHG materials.

摘要

一种优异的二次谐波产生(SHG)材料,即锂镁碘酸盐(LiMg(IO),简称LMIO),是通过对LiM(IO)(M = Ti、Sn和Ge)中的中心M阳离子进行异价取代并随后进行Wyckoff位置交换而精心设计出来的。新结构维持了(IO)基团的理想排列。重要的是,LMIO在1064 nm激光辐射下表现出约为24×KHPO(KDP)的极强SHG效应,或者在2.05 μm激光辐射下表现出1.5×AgGaS(AGS)的SHG效应,这比α-LiIO(18×KDP)的效应更大。用Mg取代M且不存在d-d电子跃迁会导致明显更大的带隙(4.34 eV)以及较短的吸收边(285 nm)。这项研究表明,单位点异价取代为设计SHG材料提供了一条新的合成途径。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/94d1b8f18281/c9sc04832d-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/12d95d0bb255/c9sc04832d-f1.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/8b476bdf526e/c9sc04832d-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/67dae48e7a04/c9sc04832d-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/bb8b5476d62f/c9sc04832d-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/94d1b8f18281/c9sc04832d-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/12d95d0bb255/c9sc04832d-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/81cf23a58cdb/c9sc04832d-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/8b476bdf526e/c9sc04832d-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/67dae48e7a04/c9sc04832d-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/bb8b5476d62f/c9sc04832d-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/33eb/7066663/94d1b8f18281/c9sc04832d-f6.jpg

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