Zihao Shao , Yuerong Bai , Dechun Zhou , Zhuang Leng , Kexuan Han , Fengjie Qin
{"title":"Structure network topology and broadband 2.7 μm luminescence in Er3+/Pr3+ co-doped TeO2-BaF2-YF3 glass","authors":"Zihao Shao , Yuerong Bai , Dechun Zhou , Zhuang Leng , Kexuan Han , Fengjie Qin","doi":"10.1016/j.ceramint.2025.01.584","DOIUrl":null,"url":null,"abstract":"<div><div>In this paper, Er<sup>3+</sup>/Pr<sup>3+</sup> co-doped tellurite fluoride glass samples were prepared by high-temperature melting method, and the structural and optical properties of the glass samples were investigated and discussed by Raman spectroscopy, DSC mapping, absorption spectroscopy, and fluorescence spectroscopy with a view to obtaining a gain medium with good luminescence performance for the 2.7 μm band. The results of Raman spectroscopy show that the glass has a maximum phonon energy of 755 cm<sup>−1</sup>. The lower maximum phonon energy is attributed to the introduction of F<sup>−</sup>, which leads to the breakage of the Te-O-Te bond in the structure and the formation of two kinds of bonds, O-Te-F and Te-F-Te, which makes the structure of TeO<sub>4</sub> gradually transformed into TeO<sub>3+1</sub> and TeO<sub>3</sub>, and the fluoride–tellurite crystal system presents two phases of oxyfluoride (TeO<sub>3</sub>F<sub>2</sub> and TeOF<sub>2</sub>) based on the formation of α and β TeO<sub>2</sub> polymorphs. On the other hand, the change of structure network topology effectively inhibits the interaction between rare earth ions and reduces their nonradiative transitions probabilities, which provides a powerful environment for the mid-infrared band luminescence thus enhancing the infrared luminescence performance. The DSC pattern shows that the glass has a T<sub>g</sub> of 355 °C and a ΔT as high as 118 °C, which suggests that the glass has a good thermal stability. The fluorescence spectra show that when the doping concentration of Er<sub>2</sub>O<sub>3</sub>/PrF<sub>3</sub> is 1 mol% and 2 mol%, the maximum fluorescence intensity of 2.7 μm is acquired. The fluorescence half-height width of the glass is 138 nm, and the effective fluorescence bandwidth of the glass is <span><math><mrow><mo>Δ</mo><msub><mi>λ</mi><mrow><mi>e</mi><mi>f</mi><mi>f</mi></mrow></msub></mrow></math></span> = 147.4 nm, which is a sufficient guarantee for the realization of the tunable laser of 2.7 μm with a wide <span><math><mrow><mo>Δ</mo><msub><mi>λ</mi><mrow><mi>e</mi><mi>f</mi><mi>f</mi></mrow></msub></mrow></math></span>. The Judd-Ofelt intensity parameters were calculated by combining the absorption spectra, where the Ω<sub>2</sub>,Ω<sub>4</sub>,Ω<sub>6</sub>, and spectral quality factor (χ = Ω<sub>4</sub>/Ω<sub>6</sub>) of the glass were 6.83 × 10<sup>−20</sup> cm<sup>2</sup>, 2.49 × 10<sup>−20</sup> cm<sup>2</sup>,1.78 × 10<sup>−20</sup> cm<sup>2</sup>, and 1.40, respectively. Meanwhile, the emission cross-section reached 6.37 × 10<sup>−21</sup> cm<sup>2</sup>, with maximum gain coefficients of 2.28 cm<sup>−1</sup>, indicating that the glass sample has a low lasing threshold and is expected to produce efficient 2.7 μm luminescence. The results indicate that the Er<sup>3+</sup>/Pr<sup>3+</sup> co-doped 70TeO<sub>2</sub>-20BaF<sub>2</sub>-10YF<sub>3</sub> glass is a promising laser glass material in the 2.7 μm band.</div></div>","PeriodicalId":267,"journal":{"name":"Ceramics International","volume":"51 13","pages":"Pages 18086-18094"},"PeriodicalIF":5.1000,"publicationDate":"2025-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Ceramics International","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0272884225006418","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATERIALS SCIENCE, CERAMICS","Score":null,"Total":0}
引用次数: 0
Abstract
In this paper, Er3+/Pr3+ co-doped tellurite fluoride glass samples were prepared by high-temperature melting method, and the structural and optical properties of the glass samples were investigated and discussed by Raman spectroscopy, DSC mapping, absorption spectroscopy, and fluorescence spectroscopy with a view to obtaining a gain medium with good luminescence performance for the 2.7 μm band. The results of Raman spectroscopy show that the glass has a maximum phonon energy of 755 cm−1. The lower maximum phonon energy is attributed to the introduction of F−, which leads to the breakage of the Te-O-Te bond in the structure and the formation of two kinds of bonds, O-Te-F and Te-F-Te, which makes the structure of TeO4 gradually transformed into TeO3+1 and TeO3, and the fluoride–tellurite crystal system presents two phases of oxyfluoride (TeO3F2 and TeOF2) based on the formation of α and β TeO2 polymorphs. On the other hand, the change of structure network topology effectively inhibits the interaction between rare earth ions and reduces their nonradiative transitions probabilities, which provides a powerful environment for the mid-infrared band luminescence thus enhancing the infrared luminescence performance. The DSC pattern shows that the glass has a Tg of 355 °C and a ΔT as high as 118 °C, which suggests that the glass has a good thermal stability. The fluorescence spectra show that when the doping concentration of Er2O3/PrF3 is 1 mol% and 2 mol%, the maximum fluorescence intensity of 2.7 μm is acquired. The fluorescence half-height width of the glass is 138 nm, and the effective fluorescence bandwidth of the glass is = 147.4 nm, which is a sufficient guarantee for the realization of the tunable laser of 2.7 μm with a wide . The Judd-Ofelt intensity parameters were calculated by combining the absorption spectra, where the Ω2,Ω4,Ω6, and spectral quality factor (χ = Ω4/Ω6) of the glass were 6.83 × 10−20 cm2, 2.49 × 10−20 cm2,1.78 × 10−20 cm2, and 1.40, respectively. Meanwhile, the emission cross-section reached 6.37 × 10−21 cm2, with maximum gain coefficients of 2.28 cm−1, indicating that the glass sample has a low lasing threshold and is expected to produce efficient 2.7 μm luminescence. The results indicate that the Er3+/Pr3+ co-doped 70TeO2-20BaF2-10YF3 glass is a promising laser glass material in the 2.7 μm band.
期刊介绍:
Ceramics International covers the science of advanced ceramic materials. The journal encourages contributions that demonstrate how an understanding of the basic chemical and physical phenomena may direct materials design and stimulate ideas for new or improved processing techniques, in order to obtain materials with desired structural features and properties.
Ceramics International covers oxide and non-oxide ceramics, functional glasses, glass ceramics, amorphous inorganic non-metallic materials (and their combinations with metal and organic materials), in the form of particulates, dense or porous bodies, thin/thick films and laminated, graded and composite structures. Process related topics such as ceramic-ceramic joints or joining ceramics with dissimilar materials, as well as surface finishing and conditioning are also covered. Besides traditional processing techniques, manufacturing routes of interest include innovative procedures benefiting from externally applied stresses, electromagnetic fields and energetic beams, as well as top-down and self-assembly nanotechnology approaches. In addition, the journal welcomes submissions on bio-inspired and bio-enabled materials designs, experimentally validated multi scale modelling and simulation for materials design, and the use of the most advanced chemical and physical characterization techniques of structure, properties and behaviour.
Technologically relevant low-dimensional systems are a particular focus of Ceramics International. These include 0, 1 and 2-D nanomaterials (also covering CNTs, graphene and related materials, and diamond-like carbons), their nanocomposites, as well as nano-hybrids and hierarchical multifunctional nanostructures that might integrate molecular, biological and electronic components.