{"title":"三相ZrO2纳米颗粒中的电子阱能量分布及其剂量学特性","authors":"J.M. Kalita , M.L. Chithambo","doi":"10.1016/j.jlumin.2025.121554","DOIUrl":null,"url":null,"abstract":"<div><div>Electron trap energy distribution in ZrO<sub>2</sub> prepared by wet chemical synthesis is studied using thermoluminescence (TL). The sample has 70 % monoclinic phase ZrO<sub>2</sub>, 25 % cubic phase ZrO<sub>2</sub> and 5 % tetragonal phase ZrO<sub>2</sub>. The morphology of its grains is spherical with average size 18.5 ± 3.5 nm as determined by a field-emission scanning electron microscopy. A TL glow curve recorded at 1 <sup>o</sup>C/s following beta irradiation to 10 Gy has an apparently single peak near 75 °C. Kinetic analysis of this glow peak reveals that the peak is composed of several overlapping components. The activation energies of these components lie between 0.40 and 0.80 eV. The activation energies associated with the component traps follow a Gaussian distribution with the maximum at 0.57 ± 0.01 eV and a width of 0.11 ± 0.01 eV. The glow peak shows sublinear dose response between 1 and 15 Gy with the superlinearity index <em>g</em>(<em>D</em>) equal to 0.92 ± 0.01. The glow peak fades with delay between irradiation and measurement. The intensity, noted as peak height decreases by half about 1670 s after irradiation. The glow peak is reproducible. The coefficient of variation of the peak position, peak height and peak area in 20 identical measurements are 1.39, 0.95 and 0.62 % respectively. The TL is attributed to oxygen vacancies (F and F<sup>+</sup> centres) and intrinsic Ti<sup>3+</sup> impurities.</div></div>","PeriodicalId":16159,"journal":{"name":"Journal of Luminescence","volume":"288 ","pages":"Article 121554"},"PeriodicalIF":3.6000,"publicationDate":"2025-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Electron trap energy distribution in triphasic ZrO2 nanoparticle and its dosimetric characteristics\",\"authors\":\"J.M. Kalita , M.L. Chithambo\",\"doi\":\"10.1016/j.jlumin.2025.121554\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Electron trap energy distribution in ZrO<sub>2</sub> prepared by wet chemical synthesis is studied using thermoluminescence (TL). The sample has 70 % monoclinic phase ZrO<sub>2</sub>, 25 % cubic phase ZrO<sub>2</sub> and 5 % tetragonal phase ZrO<sub>2</sub>. The morphology of its grains is spherical with average size 18.5 ± 3.5 nm as determined by a field-emission scanning electron microscopy. A TL glow curve recorded at 1 <sup>o</sup>C/s following beta irradiation to 10 Gy has an apparently single peak near 75 °C. Kinetic analysis of this glow peak reveals that the peak is composed of several overlapping components. The activation energies of these components lie between 0.40 and 0.80 eV. The activation energies associated with the component traps follow a Gaussian distribution with the maximum at 0.57 ± 0.01 eV and a width of 0.11 ± 0.01 eV. The glow peak shows sublinear dose response between 1 and 15 Gy with the superlinearity index <em>g</em>(<em>D</em>) equal to 0.92 ± 0.01. The glow peak fades with delay between irradiation and measurement. The intensity, noted as peak height decreases by half about 1670 s after irradiation. The glow peak is reproducible. The coefficient of variation of the peak position, peak height and peak area in 20 identical measurements are 1.39, 0.95 and 0.62 % respectively. The TL is attributed to oxygen vacancies (F and F<sup>+</sup> centres) and intrinsic Ti<sup>3+</sup> impurities.</div></div>\",\"PeriodicalId\":16159,\"journal\":{\"name\":\"Journal of Luminescence\",\"volume\":\"288 \",\"pages\":\"Article 121554\"},\"PeriodicalIF\":3.6000,\"publicationDate\":\"2025-09-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Luminescence\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0022231325004946\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Luminescence","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0022231325004946","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"OPTICS","Score":null,"Total":0}
Electron trap energy distribution in triphasic ZrO2 nanoparticle and its dosimetric characteristics
Electron trap energy distribution in ZrO2 prepared by wet chemical synthesis is studied using thermoluminescence (TL). The sample has 70 % monoclinic phase ZrO2, 25 % cubic phase ZrO2 and 5 % tetragonal phase ZrO2. The morphology of its grains is spherical with average size 18.5 ± 3.5 nm as determined by a field-emission scanning electron microscopy. A TL glow curve recorded at 1 oC/s following beta irradiation to 10 Gy has an apparently single peak near 75 °C. Kinetic analysis of this glow peak reveals that the peak is composed of several overlapping components. The activation energies of these components lie between 0.40 and 0.80 eV. The activation energies associated with the component traps follow a Gaussian distribution with the maximum at 0.57 ± 0.01 eV and a width of 0.11 ± 0.01 eV. The glow peak shows sublinear dose response between 1 and 15 Gy with the superlinearity index g(D) equal to 0.92 ± 0.01. The glow peak fades with delay between irradiation and measurement. The intensity, noted as peak height decreases by half about 1670 s after irradiation. The glow peak is reproducible. The coefficient of variation of the peak position, peak height and peak area in 20 identical measurements are 1.39, 0.95 and 0.62 % respectively. The TL is attributed to oxygen vacancies (F and F+ centres) and intrinsic Ti3+ impurities.
期刊介绍:
The purpose of the Journal of Luminescence is to provide a means of communication between scientists in different disciplines who share a common interest in the electronic excited states of molecular, ionic and covalent systems, whether crystalline, amorphous, or liquid.
We invite original papers and reviews on such subjects as: exciton and polariton dynamics, dynamics of localized excited states, energy and charge transport in ordered and disordered systems, radiative and non-radiative recombination, relaxation processes, vibronic interactions in electronic excited states, photochemistry in condensed systems, excited state resonance, double resonance, spin dynamics, selective excitation spectroscopy, hole burning, coherent processes in excited states, (e.g. coherent optical transients, photon echoes, transient gratings), multiphoton processes, optical bistability, photochromism, and new techniques for the study of excited states. This list is not intended to be exhaustive. Papers in the traditional areas of optical spectroscopy (absorption, MCD, luminescence, Raman scattering) are welcome. Papers on applications (phosphors, scintillators, electro- and cathodo-luminescence, radiography, bioimaging, solar energy, energy conversion, etc.) are also welcome if they present results of scientific, rather than only technological interest. However, papers containing purely theoretical results, not related to phenomena in the excited states, as well as papers using luminescence spectroscopy to perform routine analytical chemistry or biochemistry procedures, are outside the scope of the journal. Some exceptions will be possible at the discretion of the editors.