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The broad hump in the diffraction pattern specified the amorphous behaviour of the TZP glass. The various vibrational shoulder linkages were characterized using the Fourier transform infrared (FT\u2010IR) spectroscopy. The optical absorption spectrum was measured in the ultraviolet (UV)\u2013visible (Vis) light region for the Eu<jats:sup>3+<\/jats:sup>\u2010doped TZP (TZPE) glass and the optical band gap was found to be 3.12\u2009eV. Eu<jats:sup>3+<\/jats:sup>\u2010doped TZP glasses showed several emission peaks in the visible region including an intense red emission peak due to the <jats:sup>5<\/jats:sup>D<jats:sub>0<\/jats:sub>\u2192<jats:sup>7<\/jats:sup>F<jats:sub>2<\/jats:sub> transition under an excitation wavelength of \u03bb<jats:sub>ex<\/jats:sub>\u00a0=\u2009393\u2009nm, which was matched with the emitting wavelength of the near\u2010UV LED chip. Commission Internationale de I'Eclairage (CIE)\u00a0chromaticity coordinates were situated in the red region and nearly matched with the coordinates of the commercial red phosphor (Y<jats:sub>2<\/jats:sub>O<jats:sub>3<\/jats:sub>S:Eu<jats:sup>3+<\/jats:sup>). The decay profile of the TZPE50 glass exhibited a single exponential fit with a decay time (\n of 1.76\u2009ms. Temperature\u2010dependent photoluminescence (TDPL) studies demonstrate\u00a0that the as\u2010prepared glass consist of excellent thermal stability. The detailed analysis and results confirmed that the red\u2010emitting TZPE glasses were potential candidates for white\u2010LED and other photonic applications.<\/jats:p>","DOI":"10.1002\/bio.4391","type":"journal-article","created":{"date-parts":[[2022,10,7]],"date-time":"2022-10-07T05:44:35Z","timestamp":1665121475000},"page":"2059-2066","update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":9,"title":["Thermally stable red luminescence from Eu<sup>3+<\/sup>\u2010activated telluro zinc phosphate glass under near\u2010ultraviolet light excitation for photonic applications"],"prefix":"10.1002","volume":"37","author":[{"family":"Vikas","sequence":"first","affiliation":[{"name":"Luminescent Materials Research Laboratory (LMRL), Department of Applied Physics Delhi Technological University  Delhi India"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-3459-1473","authenticated-orcid":false,"given":"Mula","family":"Jayasimhadri","sequence":"additional","affiliation":[{"name":"Luminescent Materials Research Laboratory (LMRL), Department of Applied Physics Delhi Technological University  Delhi India"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"311","published-online":{"date-parts":[[2022,10,25]]},"reference":[{"key":"e_1_2_7_2_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.solmat.2013.10.030"},{"key":"e_1_2_7_3_1","doi-asserted-by":"publisher","DOI":"10.1038\/lsa.2015.105"},{"key":"e_1_2_7_4_1","doi-asserted-by":"publisher","DOI":"10.1021\/ic402870p"},{"key":"e_1_2_7_5_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.matchemphys.2006.11.020"},{"key":"e_1_2_7_6_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.pmatsci.2018.11.003"},{"key":"e_1_2_7_7_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jlumin.2019.01.042"},{"key":"e_1_2_7_8_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jlumin.2013.04.006"},{"key":"e_1_2_7_9_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jlumin.2010.05.006"},{"key":"e_1_2_7_10_1","doi-asserted-by":"publisher","DOI":"10.1016\/0022-2313(91)90181-T"},{"key":"e_1_2_7_11_1","doi-asserted-by":"publisher","DOI":"10.1063\/1.3551584"},{"key":"e_1_2_7_12_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jallcom.2016.12.150"},{"key":"e_1_2_7_13_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.mser.2010.07.001"},{"key":"e_1_2_7_14_1","doi-asserted-by":"publisher","DOI":"10.1063\/1.1755025"},{"key":"e_1_2_7_15_1","doi-asserted-by":"publisher","DOI":"10.1039\/C5DT02436F"},{"key":"e_1_2_7_16_1","doi-asserted-by":"publisher","DOI":"10.1007\/s10895-015-1689-8"},{"key":"e_1_2_7_17_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.mser.2010.07.001"},{"key":"e_1_2_7_18_1","doi-asserted-by":"publisher","DOI":"10.1038\/srep03541"},{"key":"e_1_2_7_19_1","doi-asserted-by":"publisher","DOI":"10.1021\/am405228x"},{"key":"e_1_2_7_20_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jallcom.2015.05.138"},{"key":"e_1_2_7_21_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.saa.2003.12.022"},{"key":"e_1_2_7_22_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jnoncrysol.2016.08.020"},{"key":"e_1_2_7_23_1","doi-asserted-by":"publisher","DOI":"10.1111\/jace.12430"},{"key":"e_1_2_7_24_1","doi-asserted-by":"publisher","DOI":"10.1016\/S0022-3093(99)00620-1"},{"key":"e_1_2_7_25_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jallcom.2017.03.020"},{"key":"e_1_2_7_26_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.matchemphys.2005.03.035"},{"key":"e_1_2_7_27_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.jnoncrysol.2013.07.024"},{"key":"e_1_2_7_28_1","first-page":"32605","volume":"4","author":"Maheshwary B. 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