Electronic structure, morphology-controlled synthesis, and luminescence properties of YF3: Eu3

Studying electronic structure plays a key role in improving the photoluminescence (PL) properties of materials. Therefore, the electronic structure of YF 3 : x Eu 3+ with different Eu 3+ ions doping concentrations was explored by first-principles calculations based on density functional theory (DFT)...

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Veröffentlicht in:Journal of sol-gel science and technology 2021-06, Vol.98 (3), p.497-507
Hauptverfasser: Jia, Ke, Bi, Zun, Liu, Yunfei, Lyu, Yinong
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Lyu, Yinong
description Studying electronic structure plays a key role in improving the photoluminescence (PL) properties of materials. Therefore, the electronic structure of YF 3 : x Eu 3+ with different Eu 3+ ions doping concentrations was explored by first-principles calculations based on density functional theory (DFT). As calculated, the YF 3 host had an indirect bandgap of 7.68 eV. From all calculation results we got, the band structure of YF 3 : x Eu 3+ exhibited the smallest direct band gap of 6.54 eV when the value of x was 0.10. This small direct band gap is beneficial to obtain excellent emission intensity. Besides, the morphologies and sizes have a significant influence on the fluorescence intensity of the products. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio via a microwave hydrothermal method. At the same time, the formation process of granule-like YF 3 : Eu 3+ was explored through time-dependent experiments. Furthermore, the fluorescence performance of YF 3 : x Eu 3+ was studied in detail. The as-obtained YF 3 : x Eu 3+ can exhibit orange-red emission under ultraviolet excitation because of the magnetic dipole of the 5 D 0 – 7 F 1 transition of Eu 3+ ions. After comparing the luminescence properties of samples with different morphologies, we found that the sample with granule-like morphology had the highest orange-red emission intensity. The experimental result proved that the appropriate Eu 3+ ions doping concentration were x  = 0.10, which is highly consistent with the calculation result. The great orange-red emission intensity was obtained by adjusting the electronic structure and morphology of the YF 3 : x Eu 3+ . The electronic structures of YF 3 : x Eu 3+ can be altered by changing Eu 3+ doping concentrations. The morphologies can be regulated by changing the RE 3+ /NaF ratio. Besides, the formation process of granule-like YF 3 : 0.1Eu 3+ was explored through time-dependent experiments. Highlights The electronic structures of Eu 3+ -doped YF 3 phosphors were studied by DFT calculations. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio. The formation process of granule-like YF 3 : Eu 3+ was explored. The PL properties based on different morphologies and the concentration of Eu 3+ ions were studied.
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Therefore, the electronic structure of YF 3 : x Eu 3+ with different Eu 3+ ions doping concentrations was explored by first-principles calculations based on density functional theory (DFT). As calculated, the YF 3 host had an indirect bandgap of 7.68 eV. From all calculation results we got, the band structure of YF 3 : x Eu 3+ exhibited the smallest direct band gap of 6.54 eV when the value of x was 0.10. This small direct band gap is beneficial to obtain excellent emission intensity. Besides, the morphologies and sizes have a significant influence on the fluorescence intensity of the products. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio via a microwave hydrothermal method. At the same time, the formation process of granule-like YF 3 : Eu 3+ was explored through time-dependent experiments. Furthermore, the fluorescence performance of YF 3 : x Eu 3+ was studied in detail. The as-obtained YF 3 : x Eu 3+ can exhibit orange-red emission under ultraviolet excitation because of the magnetic dipole of the 5 D 0 – 7 F 1 transition of Eu 3+ ions. After comparing the luminescence properties of samples with different morphologies, we found that the sample with granule-like morphology had the highest orange-red emission intensity. The experimental result proved that the appropriate Eu 3+ ions doping concentration were x  = 0.10, which is highly consistent with the calculation result. The great orange-red emission intensity was obtained by adjusting the electronic structure and morphology of the YF 3 : x Eu 3+ . The electronic structures of YF 3 : x Eu 3+ can be altered by changing Eu 3+ doping concentrations. The morphologies can be regulated by changing the RE 3+ /NaF ratio. Besides, the formation process of granule-like YF 3 : 0.1Eu 3+ was explored through time-dependent experiments. Highlights The electronic structures of Eu 3+ -doped YF 3 phosphors were studied by DFT calculations. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio. The formation process of granule-like YF 3 : Eu 3+ was explored. The PL properties based on different morphologies and the concentration of Eu 3+ ions were studied.</description><identifier>ISSN: 0928-0707</identifier><identifier>EISSN: 1573-4846</identifier><identifier>DOI: 10.1007/s10971-021-05536-8</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Ceramics ; Chemistry and Materials Science ; colloids ; Composites ; Density functional theory ; Doping ; Electronic structure ; Emission analysis ; Emission spectra ; Energy gap ; etc. ; Europium ; fibers ; First principles ; Fluorescence ; Glass ; Granular materials ; Inorganic Chemistry ; Luminescence ; Magnetic dipoles ; Material properties ; Materials Science ; Mathematical analysis ; Morphology ; Nanotechnology ; Natural Materials ; Optical and Electronic Materials ; Optical properties ; Original Paper: Nano-structured materials (particles ; Phosphors ; Photoluminescence ; Time dependence</subject><ispartof>Journal of sol-gel science and technology, 2021-06, Vol.98 (3), p.497-507</ispartof><rights>The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021</rights><rights>The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c286t-dd3e552e08380866b15cd37dfce447753c5ab969cb0d558cf275a43222df86993</citedby><cites>FETCH-LOGICAL-c286t-dd3e552e08380866b15cd37dfce447753c5ab969cb0d558cf275a43222df86993</cites><orcidid>0000-0002-4397-6607</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s10971-021-05536-8$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s10971-021-05536-8$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27922,27923,41486,42555,51317</link.rule.ids></links><search><creatorcontrib>Jia, Ke</creatorcontrib><creatorcontrib>Bi, Zun</creatorcontrib><creatorcontrib>Liu, Yunfei</creatorcontrib><creatorcontrib>Lyu, Yinong</creatorcontrib><title>Electronic structure, morphology-controlled synthesis, and luminescence properties of YF3: Eu3</title><title>Journal of sol-gel science and technology</title><addtitle>J Sol-Gel Sci Technol</addtitle><description>Studying electronic structure plays a key role in improving the photoluminescence (PL) properties of materials. Therefore, the electronic structure of YF 3 : x Eu 3+ with different Eu 3+ ions doping concentrations was explored by first-principles calculations based on density functional theory (DFT). As calculated, the YF 3 host had an indirect bandgap of 7.68 eV. From all calculation results we got, the band structure of YF 3 : x Eu 3+ exhibited the smallest direct band gap of 6.54 eV when the value of x was 0.10. This small direct band gap is beneficial to obtain excellent emission intensity. Besides, the morphologies and sizes have a significant influence on the fluorescence intensity of the products. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio via a microwave hydrothermal method. At the same time, the formation process of granule-like YF 3 : Eu 3+ was explored through time-dependent experiments. Furthermore, the fluorescence performance of YF 3 : x Eu 3+ was studied in detail. The as-obtained YF 3 : x Eu 3+ can exhibit orange-red emission under ultraviolet excitation because of the magnetic dipole of the 5 D 0 – 7 F 1 transition of Eu 3+ ions. After comparing the luminescence properties of samples with different morphologies, we found that the sample with granule-like morphology had the highest orange-red emission intensity. The experimental result proved that the appropriate Eu 3+ ions doping concentration were x  = 0.10, which is highly consistent with the calculation result. The great orange-red emission intensity was obtained by adjusting the electronic structure and morphology of the YF 3 : x Eu 3+ . The electronic structures of YF 3 : x Eu 3+ can be altered by changing Eu 3+ doping concentrations. The morphologies can be regulated by changing the RE 3+ /NaF ratio. Besides, the formation process of granule-like YF 3 : 0.1Eu 3+ was explored through time-dependent experiments. Highlights The electronic structures of Eu 3+ -doped YF 3 phosphors were studied by DFT calculations. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio. The formation process of granule-like YF 3 : Eu 3+ was explored. The PL properties based on different morphologies and the concentration of Eu 3+ ions were studied.</description><subject>Ceramics</subject><subject>Chemistry and Materials Science</subject><subject>colloids</subject><subject>Composites</subject><subject>Density functional theory</subject><subject>Doping</subject><subject>Electronic structure</subject><subject>Emission analysis</subject><subject>Emission spectra</subject><subject>Energy gap</subject><subject>etc.</subject><subject>Europium</subject><subject>fibers</subject><subject>First principles</subject><subject>Fluorescence</subject><subject>Glass</subject><subject>Granular materials</subject><subject>Inorganic Chemistry</subject><subject>Luminescence</subject><subject>Magnetic dipoles</subject><subject>Material properties</subject><subject>Materials Science</subject><subject>Mathematical analysis</subject><subject>Morphology</subject><subject>Nanotechnology</subject><subject>Natural Materials</subject><subject>Optical and Electronic Materials</subject><subject>Optical properties</subject><subject>Original Paper: Nano-structured materials (particles</subject><subject>Phosphors</subject><subject>Photoluminescence</subject><subject>Time dependence</subject><issn>0928-0707</issn><issn>1573-4846</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>AFKRA</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp9kDFPwzAQhS0EEqXwB5gssdZwtuPYYUNVC0iVWGBgwUptp02V2sVOhv57DEFiYzjdcO-9e_oQuqZwSwHkXaJQSUqA5RGCl0SdoAkVkpNCFeUpmkDFFAEJ8hxdpLQDAFFQOUEfi86ZPgbfGpz6OJh-iG6G9yEetqELmyMxwed71zmL09H3W5faNMO1t7gb9q13yThvHD7EcHCxb13CocHvS36PFwO_RGdN3SV39bun6G25eJ0_kdXL4_P8YUUMU2VPrOVOCOZAcQWqLNdUGMulbYwrCikFN6JeV2Vl1mCFUKZhUtQFZ4zZRpVVxafoZszNNT4Hl3q9C0P0-aVmgtOCQQWQVWxUmRhSiq7Rh9ju63jUFPQ3Rz1y1Jmj_uGoVTbx0ZSy2G9c_Iv-x_UF7152Dw</recordid><startdate>20210601</startdate><enddate>20210601</enddate><creator>Jia, Ke</creator><creator>Bi, Zun</creator><creator>Liu, Yunfei</creator><creator>Lyu, Yinong</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>AFKRA</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>KB.</scope><scope>L6V</scope><scope>M7S</scope><scope>PDBOC</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><orcidid>https://orcid.org/0000-0002-4397-6607</orcidid></search><sort><creationdate>20210601</creationdate><title>Electronic structure, morphology-controlled synthesis, and luminescence properties of YF3: Eu3</title><author>Jia, Ke ; 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Therefore, the electronic structure of YF 3 : x Eu 3+ with different Eu 3+ ions doping concentrations was explored by first-principles calculations based on density functional theory (DFT). As calculated, the YF 3 host had an indirect bandgap of 7.68 eV. From all calculation results we got, the band structure of YF 3 : x Eu 3+ exhibited the smallest direct band gap of 6.54 eV when the value of x was 0.10. This small direct band gap is beneficial to obtain excellent emission intensity. Besides, the morphologies and sizes have a significant influence on the fluorescence intensity of the products. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio via a microwave hydrothermal method. At the same time, the formation process of granule-like YF 3 : Eu 3+ was explored through time-dependent experiments. Furthermore, the fluorescence performance of YF 3 : x Eu 3+ was studied in detail. The as-obtained YF 3 : x Eu 3+ can exhibit orange-red emission under ultraviolet excitation because of the magnetic dipole of the 5 D 0 – 7 F 1 transition of Eu 3+ ions. After comparing the luminescence properties of samples with different morphologies, we found that the sample with granule-like morphology had the highest orange-red emission intensity. The experimental result proved that the appropriate Eu 3+ ions doping concentration were x  = 0.10, which is highly consistent with the calculation result. The great orange-red emission intensity was obtained by adjusting the electronic structure and morphology of the YF 3 : x Eu 3+ . The electronic structures of YF 3 : x Eu 3+ can be altered by changing Eu 3+ doping concentrations. The morphologies can be regulated by changing the RE 3+ /NaF ratio. Besides, the formation process of granule-like YF 3 : 0.1Eu 3+ was explored through time-dependent experiments. Highlights The electronic structures of Eu 3+ -doped YF 3 phosphors were studied by DFT calculations. A series of YF 3 : x Eu 3+ phosphors with leaf-like, spindle-like, pecan-like, and granular-like morphologies were obtained by changing the RE 3+ /NaF ratio. The formation process of granule-like YF 3 : Eu 3+ was explored. The PL properties based on different morphologies and the concentration of Eu 3+ ions were studied.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10971-021-05536-8</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-4397-6607</orcidid></addata></record>
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subjects Ceramics
Chemistry and Materials Science
colloids
Composites
Density functional theory
Doping
Electronic structure
Emission analysis
Emission spectra
Energy gap
etc.
Europium
fibers
First principles
Fluorescence
Glass
Granular materials
Inorganic Chemistry
Luminescence
Magnetic dipoles
Material properties
Materials Science
Mathematical analysis
Morphology
Nanotechnology
Natural Materials
Optical and Electronic Materials
Optical properties
Original Paper: Nano-structured materials (particles
Phosphors
Photoluminescence
Time dependence
title Electronic structure, morphology-controlled synthesis, and luminescence properties of YF3: Eu3
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