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Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations
Two nonlinear optical crystals, BaVO(IO(3))(5) and BaTaO(IO(3))(5), are designed by substituting Nb with V and Ta, respectively, in BaNbO(IO(3))(5), which is itself a recently synthesized infrared nonlinear optical (NLO) material. The designs of BaVO(IO(3))(5) and BaTaO(IO(3))(5) from BaNbO(IO(3))(5...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2018
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6213473/ https://www.ncbi.nlm.nih.gov/pubmed/30249992 http://dx.doi.org/10.3390/ma11101809 |
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author | Li, Yingfeng Cui, Mengqi Yan, Hejin Yu, Yangxin Li, Meicheng Li, Xiang Chu, Lihua Jiang, Bing Qin, Mingde |
author_facet | Li, Yingfeng Cui, Mengqi Yan, Hejin Yu, Yangxin Li, Meicheng Li, Xiang Chu, Lihua Jiang, Bing Qin, Mingde |
author_sort | Li, Yingfeng |
collection | PubMed |
description | Two nonlinear optical crystals, BaVO(IO(3))(5) and BaTaO(IO(3))(5), are designed by substituting Nb with V and Ta, respectively, in BaNbO(IO(3))(5), which is itself a recently synthesized infrared nonlinear optical (NLO) material. The designs of BaVO(IO(3))(5) and BaTaO(IO(3))(5) from BaNbO(IO(3))(5) are based on the following motivation: BaVO(IO(3))(5) should have a larger second-harmonic generation (SHG) coefficient than BaNbO(IO(3))(5), as V will result in a stronger second-order Jahn-Teller effect than Nb due to its smaller ion radius; at the same time, BaTaO(IO(3))(5) should have a larger laser-damage threshold, due to the fact that Ta has a smaller electronegativity leading to a greater band-gap. Established on reliable first-principle calculations, it is demonstrated that BaVO(IO(3))(5) has a much larger SHG coefficient than BaNbO(IO(3))(5) (23.42 × 10(−9) vs. 18.66 × 10(−9) esu); and BaTaO(IO(3))(5) has a significantly greater band-gap than BaNbO(IO(3))(5) (4.20 vs. 3.55 eV). Meanwhile, the absorption spectra and birefringences of both BaVO(IO(3))(5) and BaTaO(IO(3))(5) are acceptable for practice, suggesting that these two crystals can both be expected to be excellent infrared NLO materials. |
format | Online Article Text |
id | pubmed-6213473 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2018 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-62134732018-11-14 Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations Li, Yingfeng Cui, Mengqi Yan, Hejin Yu, Yangxin Li, Meicheng Li, Xiang Chu, Lihua Jiang, Bing Qin, Mingde Materials (Basel) Article Two nonlinear optical crystals, BaVO(IO(3))(5) and BaTaO(IO(3))(5), are designed by substituting Nb with V and Ta, respectively, in BaNbO(IO(3))(5), which is itself a recently synthesized infrared nonlinear optical (NLO) material. The designs of BaVO(IO(3))(5) and BaTaO(IO(3))(5) from BaNbO(IO(3))(5) are based on the following motivation: BaVO(IO(3))(5) should have a larger second-harmonic generation (SHG) coefficient than BaNbO(IO(3))(5), as V will result in a stronger second-order Jahn-Teller effect than Nb due to its smaller ion radius; at the same time, BaTaO(IO(3))(5) should have a larger laser-damage threshold, due to the fact that Ta has a smaller electronegativity leading to a greater band-gap. Established on reliable first-principle calculations, it is demonstrated that BaVO(IO(3))(5) has a much larger SHG coefficient than BaNbO(IO(3))(5) (23.42 × 10(−9) vs. 18.66 × 10(−9) esu); and BaTaO(IO(3))(5) has a significantly greater band-gap than BaNbO(IO(3))(5) (4.20 vs. 3.55 eV). Meanwhile, the absorption spectra and birefringences of both BaVO(IO(3))(5) and BaTaO(IO(3))(5) are acceptable for practice, suggesting that these two crystals can both be expected to be excellent infrared NLO materials. MDPI 2018-09-24 /pmc/articles/PMC6213473/ /pubmed/30249992 http://dx.doi.org/10.3390/ma11101809 Text en © 2018 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Li, Yingfeng Cui, Mengqi Yan, Hejin Yu, Yangxin Li, Meicheng Li, Xiang Chu, Lihua Jiang, Bing Qin, Mingde Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations |
title | Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations |
title_full | Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations |
title_fullStr | Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations |
title_full_unstemmed | Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations |
title_short | Excellent Infrared Nonlinear Optical Crystals BaMO(IO(3))(5) (M = V, Ta) Predicted by First Principle Calculations |
title_sort | excellent infrared nonlinear optical crystals bamo(io(3))(5) (m = v, ta) predicted by first principle calculations |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6213473/ https://www.ncbi.nlm.nih.gov/pubmed/30249992 http://dx.doi.org/10.3390/ma11101809 |
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