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Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation

Physical and chemical properties have been studied in lithium niobate (LiNbO(3), LN) crystals grown by Czochralski from a boron doped melt. Optical uniformity and optical damage resistance of LiNbO(3):B crystals have been compared with control crystals of nominally pure congruent (CLN) and near-stoi...

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Autores principales: Palatnikov, Mikhail, Sidorov, Nikolay, Kadetova, Alexandra, Titov, Roman, Biryukova, Irina, Makarova, Olga, Manukovskaya, Diana, Teplyakova, Natalya, Efremov, Ilja
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9864121/
https://www.ncbi.nlm.nih.gov/pubmed/36676468
http://dx.doi.org/10.3390/ma16020732
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author Palatnikov, Mikhail
Sidorov, Nikolay
Kadetova, Alexandra
Titov, Roman
Biryukova, Irina
Makarova, Olga
Manukovskaya, Diana
Teplyakova, Natalya
Efremov, Ilja
author_facet Palatnikov, Mikhail
Sidorov, Nikolay
Kadetova, Alexandra
Titov, Roman
Biryukova, Irina
Makarova, Olga
Manukovskaya, Diana
Teplyakova, Natalya
Efremov, Ilja
author_sort Palatnikov, Mikhail
collection PubMed
description Physical and chemical properties have been studied in lithium niobate (LiNbO(3), LN) crystals grown by Czochralski from a boron doped melt. Optical uniformity and optical damage resistance of LiNbO(3):B crystals have been compared with control crystals of nominally pure congruent (CLN) and near-stoichiometric (NSLN K(2)O) composition. LiNbO(3):B crystals structure has been studied. Studied LiNbO(3):B crystals have been grown from differently synthesized charges. The charges have been synthesized from a mixture Nb(2)O(5):B-Li(2)CO(3) using homogeneously doped Nb(2)O(5):B precursor (sample 1, (B) = 0.0034 wt% in the charge) and by a direct solid phase synthesis from Nb(2)O(5)-Li(2)CO(3)-H(3)BO(3) mixture (sample 2, (B) = 0.0079 wt% in the charge). Only traces of boron (10(−5)–10(−4) wt%) have been detected in the samples. We have established that concentration of anti-site defects Nb(Li) is lower in both LiNbO(3):B than in CLN crystals. XRD analysis has confirmed that B(3+) cations localize in faces of tetrahedral voids O(4) of LN structure. The voids act as buffers at the anion sublattice distortion. Sample 1 has been shown to have a structure closer to NSLN K(2)O crystal than sample 2. We have also shown that the chemical purity of LN crystal increases compared to the melt purity because boron creates strong compounds with impurities in the melt system Li(2)O-Nb(2)O(5)-B(2)O(3). Metals impurities thus stay in the melt and do not transfer to the crystal.
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spelling pubmed-98641212023-01-22 Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation Palatnikov, Mikhail Sidorov, Nikolay Kadetova, Alexandra Titov, Roman Biryukova, Irina Makarova, Olga Manukovskaya, Diana Teplyakova, Natalya Efremov, Ilja Materials (Basel) Article Physical and chemical properties have been studied in lithium niobate (LiNbO(3), LN) crystals grown by Czochralski from a boron doped melt. Optical uniformity and optical damage resistance of LiNbO(3):B crystals have been compared with control crystals of nominally pure congruent (CLN) and near-stoichiometric (NSLN K(2)O) composition. LiNbO(3):B crystals structure has been studied. Studied LiNbO(3):B crystals have been grown from differently synthesized charges. The charges have been synthesized from a mixture Nb(2)O(5):B-Li(2)CO(3) using homogeneously doped Nb(2)O(5):B precursor (sample 1, (B) = 0.0034 wt% in the charge) and by a direct solid phase synthesis from Nb(2)O(5)-Li(2)CO(3)-H(3)BO(3) mixture (sample 2, (B) = 0.0079 wt% in the charge). Only traces of boron (10(−5)–10(−4) wt%) have been detected in the samples. We have established that concentration of anti-site defects Nb(Li) is lower in both LiNbO(3):B than in CLN crystals. XRD analysis has confirmed that B(3+) cations localize in faces of tetrahedral voids O(4) of LN structure. The voids act as buffers at the anion sublattice distortion. Sample 1 has been shown to have a structure closer to NSLN K(2)O crystal than sample 2. We have also shown that the chemical purity of LN crystal increases compared to the melt purity because boron creates strong compounds with impurities in the melt system Li(2)O-Nb(2)O(5)-B(2)O(3). Metals impurities thus stay in the melt and do not transfer to the crystal. MDPI 2023-01-11 /pmc/articles/PMC9864121/ /pubmed/36676468 http://dx.doi.org/10.3390/ma16020732 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/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 (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Palatnikov, Mikhail
Sidorov, Nikolay
Kadetova, Alexandra
Titov, Roman
Biryukova, Irina
Makarova, Olga
Manukovskaya, Diana
Teplyakova, Natalya
Efremov, Ilja
Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation
title Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation
title_full Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation
title_fullStr Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation
title_full_unstemmed Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation
title_short Growing, Structure and Optical Properties of LiNbO(3):B Crystals, a Material for Laser Radiation Transformation
title_sort growing, structure and optical properties of linbo(3):b crystals, a material for laser radiation transformation
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9864121/
https://www.ncbi.nlm.nih.gov/pubmed/36676468
http://dx.doi.org/10.3390/ma16020732
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