Cargando…
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...
Autores principales: | , , , , , , , , |
---|---|
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 |
_version_ | 1784590838986178560 |
---|---|
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). |
format | Online Article Text |
id | pubmed-8549788 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
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 |
work_keys_str_mv | AT lishuaishuai ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT liuxiaomeng ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT wuhongping ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT songzhongfu ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT yuhongwei ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT linzheshuai ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT huzhanggui ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT wangjiyang ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate AT wuyicheng ba4cab2o52f2pconjugationofb2o5intheplanarpentagonallayerachievinglargesecondharmonicgenerationofpyroborate |