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    <identifier>10.57760/sciencedb.06920</identifier>
    <datestamp>2022-12-20T12:15:30Z</datestamp>
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<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:date>2022-12-20</dc:date>
  <dc:title>Broadband near-infrared luminescence in Erbium ions single-doping tellurite glass for optical amplification</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.06920</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>This letter proposes a facile approach for the realization of a broadband near-infrared luminescence source in erbium-ion single-doping tellurite glass, which is bent on tailoring the network structure. Under the collective action of multiple broadening mechanisms and fluorescence capture, broadband fluorescence with a full width at half maximum (FWHM) of 132 nm (1500&amp;ndash;1632 nm) was achieved. To the best of our knowledge, this is the largest FWHM reported for erbium single-doping tellurite glass materials. Meanwhile, this fiberglass exhibits excellent thermal stability and high visible to near-infrared transmittance. Furthermore, a novel equivalent 5-level Stark splitting model is proposed, which can effectively explain the spectrum broadening. This study is beneficial for the further development of broadband optical amplification.In this study, erbium-ion single-doping tellurite glass was synthesized using the conventional melt-quenching method for mol% compositions of 70TeO2-10ZnO- (20-x) WO3-xNb2O5 (x = 0, 1, 3, 5, 7, 10), referred to as Samples A0, A1, A2, A3, A4, and A5, respectively. Additionally, tellurite glass doped with a high concentration of RE ions was also prepared with elementary molar compositions of 70TeO2-10ZnO-15WO3-5Nb2O5-2Er2O3, which was denoted as Sample B. The chemical raw materials mentioned above were high-purity (99.99%) reagents. Batches of 20-gram mixtures were poured into an alumina crucible and then heated in an electronic furnace at a temperature of approximately 900 &amp;deg;C in an air atmosphere for 40 min. Subsequently, the melt was quickly transferred onto a preheated stainless plate and annealed at 400 &amp;deg;C in a muffle furnace for 6 h to remove thermal stress. Finally, the samples were polished into coincident shapes and thicknesses to measure their physical and optical properties.To determine the thermal behavior of the glass matrix, TG/DTA7300 was used to acquire the differential thermal analysis (DTA) curve at a heating rate of 10 K/min. The Raman spectra of the samples were obtained using a LabRAM HR Evolution Raman Spectrometer in the wavenumber range of 300 to 1200 excited by a 633 nm laser source. The transmission spectrum spectra were measured by the UV-VIS-NIR spectrophotometer of PerkinElmer LAMBDA 750 within the range of 250&amp;ndash;2500 nm with a resolution of 1 nm. The NIR (1400&amp;ndash;1700 nm) fluorescence spectra pumped with a commercial 980 nm LD and attenuation curve recording were collected using an FLSP980 spectrometer under liquid-nitrogen cooling conditions. All measurements mentioned in this study were performed at room temperature.</dc:description>
  <dc:subject>Tellurite glass; broadband near-infrared luminescence; optical amplification</dc:subject>
  <dc:creator>Zhiming Zhou</dc:creator>
  <dc:creator>Yanchao Li</dc:creator>
  <dc:creator>Yiguang Jiang</dc:creator>
  <dc:creator>Zaiyang Wang</dc:creator>
  <dc:creator>Pengwei Yin</dc:creator>
  <dc:creator>Longfei Zhang</dc:creator>
  <dc:creator>Long Zhang</dc:creator>
  <dc:rights>PUBLIC</dc:rights>
  <dc:rights>https://creativecommons.org/publicdomain/zero/1.0/</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:publisher>Science Data Bank</dc:publisher>
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