Article(id=1263922781893308616, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1263922767154524283, articleNumber=null, orderNo=null, doi=10.14062/j.issn.0454-5648.20250560, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1752768000000, receivedDateStr=2025-07-18, revisedDate=1757952000000, revisedDateStr=2025-09-16, acceptedDate=null, acceptedDateStr=null, onlineDate=1779272273752, onlineDateStr=2026-05-20, pubDate=1764259200000, pubDateStr=2025-11-28, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1779272273752, onlineIssueDateStr=2026-05-20, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1779272273752, creator=13041195026, updateTime=1779272273752, updator=13041195026, issue=Issue{id=1263922767154524283, tenantId=1146029695717560320, journalId=1263187385517883426, year='2025', volume='54', issue='4', pageStart='1291', pageEnd='1369', issueExtLink='null', onlineDate='null', pubDate='null', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1779272270238, creator=13041195026, updateTime=1779272270238, updator=13041195026, preIssue=null, nextIssue=null, ext=null, issueFiles=null}, startPage=1299, endPage=1306, ext={EN=ArticleExt(id=1263922783944323281, articleId=1263922781893308616, tenantId=1146029695717560320, journalId=1263187385517883426, language=EN, title=Optical, Luminescence, and Scintillation Properties of Eu-Doped MgO-P
2O
5-B
2O
3 Glasses, columnId=1263922776440750662, journalTitle=Journal of the Chinese Ceramic Society, columnName=Special Issue on Advanced Glasses and Optical Materials——Research Articles, runingTitle=null, highlight=null, articleAbstract=
Introduction Scintillators are functional materials that immediately emit low-energy photons after absorbing high-energy ionizing radiations. Glasses have advantages as a material form for scintillator use, such as low manufacturing costs, ease of formability, high optical transparency, and high compositional tunability. A 6Li-glass scintillator doped with Ce is a commercial glass scintillator, and it has been used for thermal neutron detections owing to 6Li(n,α)3H neutron capture reactions. In general, the 3He counter is used in practice for neutron detections; however, the depletion of the 3He supply has driven vigorous research and development of alternative materials. 10B-contained glasses have an advantage of their large thermal neutron capture cross section (3840 barn). In this study, we focused on MgO-P2O5-B2O3 glass systems. They are composed of light elements; hence, neutron detection signals can be easily distinguished from noise due to X- and γ-rays. Furthermore, alkali-earth-embedded P2O5-B2O3 glasses realize high optical transparency with good chemical durability. As luminescence centers, Eu was selected. Eu exists in two different states: Eu2+ in reduction states and Eu3+ in oxidation states. The former shows broad emission bands with fast decay times of ~μs, whereas the latter shows sharp emission bands with slow decay times of ~ms. In general, Eu3+ is governed in the glasses prepared in an air atmosphere; however, alkali-earth-embedded P2O5-B2O3 glasses can exhibit Eu2+ owing to the localized reducing atmosphere generated by NH3 derived from the raw material (NH4H2PO4). Here, Eu-doped MgO-P2O5-B2O3 glasses with various concentrations of Eu were synthesized by the conventional melt quenching technique in air, and their optical, photoluminescence (PL), and scintillation properties were examined.
Methods Undoped and 0.1%, 0.3%, 1.0%, and 2.0% (in mole fraction) Eu-doped 25MgO-30P2O5-45B2O3 (MPB) glasses were synthesized by the melt quenching method. Raw materials were homogeneously mixed and transferred into an alumina crucible. The powders were melted at 1100 ℃ for 1 h with an electrical furnace in air. The melt was flowed onto a preheated stainless-steel plate to quench, and pressed into batches. After that, the glasses were annealed at 400 ℃ for 1 h to remove thermal and mechanical strains. The surfaces of the glasses were polished for the following optical and scintillation measurements. The glass transition temperature (Tg) of the undoped sample was measured with a TG-DTA system. The powder X-ray diffraction (XRD) patterns were measured using a diffractometer. Diffuse transmission spectra were measured using a spectrophotometer (Shimadzu, SolidSpec-3700). PL excitation and emission spectra, PL quantum yields (QYs), and PL decay curves were measured using a Quantaurus-QY and Quantaurus-τ. Scintillation spectra, scintillation decay curves, and afterglow curves under X-ray irradiations, and pulse height spectra of 241Amα-rays and 137Cs γ-rays were measured with our original setups.
Results and discussion The appearances of undoped and Eu-doped MPB glasses were transparent and included some bubbles. Under ultraviolet light at 360 nm, Eu-doped samples showed bluish-red light. Some parts of the glasses were crushed into powder and used for the XRD measurements. Precipitations of crystalline phases were not observed in the XRD patterns; hence, the prepared samples formed glass phases with no periodical structures. Tg of the undoped glass was estimated to be 535 ℃. The transmittances of all the glasses were 70%-90% at 400-700 nm. Both the undoped and Eu-doped samples showed absorption peaks at 200-250 nm; hence, this can be due to the hosts. In addition, absorption peaks emerged at 250-400 nm in Eu-doped samples. The absorption bands at 250-280 nm and 280-400 nm originated from the 4f7-4f65d1 (T2g and Eg) transitions of Eu2+, respectively. An absorption peak due to the 7F1-5D3 transitions of Eu3+ was confirmed at 415 nm in the spectra of 2% Eu. A broad emission band due to the electronic transitions of Eu2+ was observed at 400-600 nm under excitation bands at 250-410 nm in the Eu-doped samples. Generally, emissions due to Eu2+ are difficult to observe in the glasses prepared in air because of the oxidizing atmosphere. The emissions appeared owing to the localized reduction atmosphere, which derived from NH4H2PO4 and (NH4)2O·5B2O3·8H2O. When excitation and monitored wavelengths were respectively set to 340 nm and 420 nm, the PL decay curves were fitted by a sum of two exponential functions. The PL decay time constants of both the fast (0.2-0.5 μs) and slow (0.7-1.2 μs) components were similar to those of other Eu-doped phosphors; hence, they are reasonable as 4f65d1(T2g)-4f7 and 4f65d1(Eg)-4f7 transitions of Eu2+. Eu-doped samples showed emission peaks at 350-500 nm under X-ray irradiations. These emission wavelengths were consistent with those of the PL spectra. Afterglow levels (AL) of undoped and 0.1%, 0.3%, 1.0%, and 2.0% Eu-doped glasses at 20 ms passed after X-ray irradiation of 2 ms were respectively estimated to be 1700×10-6, 4500×10-6, 3400×10-6, 800×10-6, and 160×10-6. Pulse height spectra of 241Am α-rays (5.5 MeV) were measured using the prepared MPB glasses. Eu-doped glasses showed clear full energy absorption peaks. Light yields (LY) of 0.3%, 1.0%, and 2.0% Eu-doped MPB glasses were respectively calculated to be 70, 150 photons/5.5 MeV, and 40 photons/5.5 MeV.
Conclusion Eu-doped MPB glasses were synthesized by the conventional melt quenching method. All the samples showed halo peaks with no periodic patterns in XRD measurements. The transmittances were 70%-90%, and absorptions due to electronic transitions of Eu2+ and Eu3+ were observed. All the samples showed luminescence, which originated from the 4f65d1-4f7 transitions of Eu2+. PL QYs of 0.1%, 0.3%, 1.0%, and 2.0% Eu-doped samples were respectively calculated to be 46.7%, 37.2%, 20.4%, and 9.3% when monitored at 350-560 nm under excitation at 320 nm. ALs at 20 ms passed after X-ray irradiations of 2 ms were obtained to be 1700×10-6, 4500×10-6, 3400×10-6, 800×10-6, and 160×10-6 in undoped, 0.1%, 0. 3%, 1.0%, and 2.0% Eu-doped samples, respectively. Pulse height spectra of 241Am α-rays were measured using the prepared samples. LYs of 0.3%, 1.0%, and 2.0% Eu-doped samples were respectively determined to be 70, 150 photons/5.5 MeV, and 40 photons/5.5 MeV.
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2O
5-B
2O
3玻璃的光学、发光和闪烁性能, columnId=1263922781230645866, journalTitle=硅酸盐学报, columnName=先进玻璃与光学材料专题——研究论文, runingTitle=null, highlight=null, articleAbstract=
通过熔融淬火法制备了未掺杂和掺杂Eu的MgO-P2O5-B2O3玻璃,并研究了它们的光学和闪烁性能。制备的样品具有70%~90%的透射率。由于在紫外-可见光和X射线下Eu2+发生4f65d1-4f7跃迁并产生发光。当在320 nm激发、在350~560 nm监测时0.1%、0.3%、1.0%和2.0%(摩尔分数)Eu掺杂的MgO-P2O5-B2O3玻璃的光致发光量子产率分别为46.7%、37.2%、20.4%和9.3%。在未掺杂、0.1%、0.3%、1.0%和2.0%掺杂Eu的样品中,计算出在2 ms X射线照射后20 ms的余辉水平分别为1700×10-6、4500×10-6、3400×10-6、800×10-6和160×10-6。使用合成的MgO-P2O5-B2O3玻璃测量241Am α射线脉冲高度谱。根据比较样品和参照物(Gd2SiO5、LY:8000光子/MeV)的全吸收峰位置,0.3%、1.0%和2.0%掺铕样品的光产额(LY)计算分别为70、150和40个光子/5.5 MeV。
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KAI Okazaki(1998—),男,博士研究生。
KAI Okazaki (1998-), male, Doctoral candidate. E-mail: okazaki.kai.of0@ms.naist.jp
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KAI Okazaki(1998—),男,博士研究生。
KAI Okazaki (1998-), male, Doctoral candidate. E-mail: okazaki.kai.of0@ms.naist.jp
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