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Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate

The nonlinear optical (NLO) crystals that can expand the wavelength of the laser to the deep-ultraviolet (DUV) region by the cascaded second harmonic generation (SHG) are of current research interest. It is well known that borates are the most ideal material class for the design of new DUV NLO cryst...

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Autores principales: Li, Shuaishuai, Liu, Xiaomeng, Wu, Hongping, Song, Zhongfu, Yu, Hongwei, Lin, Zheshuai, Hu, Zhanggui, Wang, Jiyang, Wu, Yicheng
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8549788/
https://www.ncbi.nlm.nih.gov/pubmed/34760175
http://dx.doi.org/10.1039/d1sc04913e
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author Li, Shuaishuai
Liu, Xiaomeng
Wu, Hongping
Song, Zhongfu
Yu, Hongwei
Lin, Zheshuai
Hu, Zhanggui
Wang, Jiyang
Wu, Yicheng
author_facet Li, Shuaishuai
Liu, Xiaomeng
Wu, Hongping
Song, Zhongfu
Yu, Hongwei
Lin, Zheshuai
Hu, Zhanggui
Wang, Jiyang
Wu, Yicheng
author_sort Li, Shuaishuai
collection PubMed
description The nonlinear optical (NLO) crystals that can expand the wavelength of the laser to the deep-ultraviolet (DUV) region by the cascaded second harmonic generation (SHG) are of current research interest. It is well known that borates are the most ideal material class for the design of new DUV NLO crystals owing to the presence of good NLO genes, e.g., BO(3) or B(3)O(6) groups. However, the NLO pyro-borates with the B(2)O(5) dimers as the sole basic building units are still rarely reported owing to their small SHG responses. In this communication, by constructing a planar pentagonal [Ca(B(2)O(5))](∞) layer, the NLO pyro-borate Ba(4)Ca(B(2)O(5))(2)F(2) with a large SHG response (∼2.2 × KDP, or ∼7 × α-Li(4)B(2)O(5)) and a DUV transparent window has been designed and synthesized. The first-principles calculations show that the large SHG response of Ba(4)Ca(B(2)O(5))(2)F(2) mainly originates from the better π-conjugation of the coplanar B(2)O(5) dimers in the [Ca(B(2)O(5))](∞) layer. In addition, the planar pentagonal pattern in the [Ca(B(2)O(5))](∞) layer provides an ideal template for designing the new DUV NLO crystals, apart from those in known DUV borates, e.g., the [Be(2)BO(3)F(2)](∞) layer in KBe(2)BO(3)F(2) (KBBF).
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spelling pubmed-85497882021-11-09 Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate Li, Shuaishuai Liu, Xiaomeng Wu, Hongping Song, Zhongfu Yu, Hongwei Lin, Zheshuai Hu, Zhanggui Wang, Jiyang Wu, Yicheng Chem Sci Chemistry The nonlinear optical (NLO) crystals that can expand the wavelength of the laser to the deep-ultraviolet (DUV) region by the cascaded second harmonic generation (SHG) are of current research interest. It is well known that borates are the most ideal material class for the design of new DUV NLO crystals owing to the presence of good NLO genes, e.g., BO(3) or B(3)O(6) groups. However, the NLO pyro-borates with the B(2)O(5) dimers as the sole basic building units are still rarely reported owing to their small SHG responses. In this communication, by constructing a planar pentagonal [Ca(B(2)O(5))](∞) layer, the NLO pyro-borate Ba(4)Ca(B(2)O(5))(2)F(2) with a large SHG response (∼2.2 × KDP, or ∼7 × α-Li(4)B(2)O(5)) and a DUV transparent window has been designed and synthesized. The first-principles calculations show that the large SHG response of Ba(4)Ca(B(2)O(5))(2)F(2) mainly originates from the better π-conjugation of the coplanar B(2)O(5) dimers in the [Ca(B(2)O(5))](∞) layer. In addition, the planar pentagonal pattern in the [Ca(B(2)O(5))](∞) layer provides an ideal template for designing the new DUV NLO crystals, apart from those in known DUV borates, e.g., the [Be(2)BO(3)F(2)](∞) layer in KBe(2)BO(3)F(2) (KBBF). The Royal Society of Chemistry 2021-09-22 /pmc/articles/PMC8549788/ /pubmed/34760175 http://dx.doi.org/10.1039/d1sc04913e Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/
spellingShingle Chemistry
Li, Shuaishuai
Liu, Xiaomeng
Wu, Hongping
Song, Zhongfu
Yu, Hongwei
Lin, Zheshuai
Hu, Zhanggui
Wang, Jiyang
Wu, Yicheng
Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate
title Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate
title_full Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate
title_fullStr Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate
title_full_unstemmed Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate
title_short Ba(4)Ca(B(2)O(5))(2)F(2): π-conjugation of B(2)O(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate
title_sort ba(4)ca(b(2)o(5))(2)f(2): π-conjugation of b(2)o(5) in the planar pentagonal layer achieving large second harmonic generation of pyro-borate
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8549788/
https://www.ncbi.nlm.nih.gov/pubmed/34760175
http://dx.doi.org/10.1039/d1sc04913e
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