{"title":"Optical studies of Dy2O3 doped phosphate glasses for potential white luminescence applications","authors":"Amel Abdallah , Chaker Bouzidi","doi":"10.1016/j.solidstatesciences.2025.107958","DOIUrl":null,"url":null,"abstract":"<div><div>Phosphate glasses with chemical compositions of (60-x) P<sub>2</sub>O<sub>5</sub>-15ZnO-15CaCO<sub>3</sub>-10Li<sub>2</sub>CO<sub>3</sub>-xDy<sub>2</sub>O<sub>3</sub> (where x = 0, 0.25, 0.5, 0.75 and 1 mol %) have been synthesized by melt quenching method. The prepared glasses were characterized by various techniques such as X-ray powder diffraction (XRD), Atomic Force Microscopy (AFM), Differential Scanning Calorimetry (DSC), Fourier Transform Infrared Spectroscopy (FTIR), photoluminescence (PL) and Judd-Ofelt (JO) theoretical model. X-ray diffraction indicates that all samples have an amorphous structure. The Atomic Force Microscopy (AFM) observation of PZCL revealed smooth surface and high quality, characterized by specific roughness parameters (R<sub>a</sub> = 2.540, R<sub>z</sub> = 11.441, R<sub>max</sub> = 13.961, R<sub>q</sub> = 3.100 nm) and presented in the form of 3D,2D surface topography. DSC measurements show that PZCLD1 have a good thermal stability among the sample and reached ΔT = 148 °C after adding Dy<sup>3+</sup>. The FTIR spectra confirming an increase of non-bridging oxygen (NBO) by addition of Dy<sub>2</sub>O<sub>3</sub>. The emission spectra presented three main bands at 491, 575 and 673 nm corresponding to the <sup>4</sup>F<sub>9/2</sub> → <sup>6</sup>H<sub>15/2</sub>, <sup>4</sup>F<sub>9/2</sub> → <sup>6</sup>H<sub>13/2</sub> and <sup>4</sup>F<sub>9/2</sub> → <sup>6</sup>H<sub>11/2</sub> transitions, respectively. The luminescence concentration quenching point is observed at 0.5 mol % of Dy<sub>2</sub>O<sub>3</sub>. The Judd–Ofelt (JO) theory was applied to the absorption bands to determine the phenomenological parameters (Ω<sub>2</sub>, Ω<sub>4</sub> and Ω<sub>6</sub> calculated subsequently). It was discovered that the JO parameters are in the following order: Ω<sub>2</sub>> Ω<sub>4</sub>> Ω<sub>6</sub>. These parameters were then used to evaluate key radiative properties, including the total spontaneous transition probability (<em>A</em><sub><em>T</em></sub>),the stimulated emission cross-section (<em>σ</em><sub><em>e</em></sub>), effective bandwidth (Δλ<sub>eff</sub>),the radiative lifetime (<em>τ</em><sub><em>rad</em></sub>) and the radiative branching ratio (<em>β</em><sub><em>rad</em></sub>) for excited luminescent states. The radiative lifetime of PZCLD0.5 τ<sub>r</sub><sub>ad</sub> = 1.31 ms calculated by Judd–Ofelt theory and experimental lifetime <span><math><mrow><mi>τ</mi></mrow></math></span><sub>exp</sub> = 0.98 ms for the level <sup>4</sup>F<sub>9/2</sub> decreases as Dy<sup>3+</sup> concentration increases. Moreover, the quantum efficiency (η = 74.80 %) of PZCLD0.5 indicates that the present material holds strong potential as a candidate for laser emission at 575 nm. The CIE coordinates is found to be x = 0.333 and y = 0.334 revealed that the present sample falls within the white region. The typical CCT value of PZCLD0.5 is estimated to be around 5471 K.</div></div>","PeriodicalId":432,"journal":{"name":"Solid State Sciences","volume":"165 ","pages":"Article 107958"},"PeriodicalIF":3.3000,"publicationDate":"2025-05-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Solid State Sciences","FirstCategoryId":"92","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1293255825001360","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, INORGANIC & NUCLEAR","Score":null,"Total":0}
引用次数: 0
Abstract
Phosphate glasses with chemical compositions of (60-x) P2O5-15ZnO-15CaCO3-10Li2CO3-xDy2O3 (where x = 0, 0.25, 0.5, 0.75 and 1 mol %) have been synthesized by melt quenching method. The prepared glasses were characterized by various techniques such as X-ray powder diffraction (XRD), Atomic Force Microscopy (AFM), Differential Scanning Calorimetry (DSC), Fourier Transform Infrared Spectroscopy (FTIR), photoluminescence (PL) and Judd-Ofelt (JO) theoretical model. X-ray diffraction indicates that all samples have an amorphous structure. The Atomic Force Microscopy (AFM) observation of PZCL revealed smooth surface and high quality, characterized by specific roughness parameters (Ra = 2.540, Rz = 11.441, Rmax = 13.961, Rq = 3.100 nm) and presented in the form of 3D,2D surface topography. DSC measurements show that PZCLD1 have a good thermal stability among the sample and reached ΔT = 148 °C after adding Dy3+. The FTIR spectra confirming an increase of non-bridging oxygen (NBO) by addition of Dy2O3. The emission spectra presented three main bands at 491, 575 and 673 nm corresponding to the 4F9/2 → 6H15/2, 4F9/2 → 6H13/2 and 4F9/2 → 6H11/2 transitions, respectively. The luminescence concentration quenching point is observed at 0.5 mol % of Dy2O3. The Judd–Ofelt (JO) theory was applied to the absorption bands to determine the phenomenological parameters (Ω2, Ω4 and Ω6 calculated subsequently). It was discovered that the JO parameters are in the following order: Ω2> Ω4> Ω6. These parameters were then used to evaluate key radiative properties, including the total spontaneous transition probability (AT),the stimulated emission cross-section (σe), effective bandwidth (Δλeff),the radiative lifetime (τrad) and the radiative branching ratio (βrad) for excited luminescent states. The radiative lifetime of PZCLD0.5 τrad = 1.31 ms calculated by Judd–Ofelt theory and experimental lifetime exp = 0.98 ms for the level 4F9/2 decreases as Dy3+ concentration increases. Moreover, the quantum efficiency (η = 74.80 %) of PZCLD0.5 indicates that the present material holds strong potential as a candidate for laser emission at 575 nm. The CIE coordinates is found to be x = 0.333 and y = 0.334 revealed that the present sample falls within the white region. The typical CCT value of PZCLD0.5 is estimated to be around 5471 K.
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