Article(id=1319971925238067338, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319971875086783028, articleNumber=null, orderNo=null, doi=10.14062/j.issn.0454-5648.20230675, pmid=null, cstr=null, oa=null, hot=null, price=null, onlineType=0, articleFormat=0, articleType=null, articleTypeStr=null, receivedDate=1693497600000, receivedDateStr=2023-09-01, revisedDate=1695571200000, revisedDateStr=2023-09-25, acceptedDate=null, acceptedDateStr=null, onlineDate=1792635430869, onlineDateStr=2026-10-22, pubDate=1710864000000, pubDateStr=2024-03-20, doiRegisterDate=null, doiRegisterDateStr=null, onlineIssueDate=1792635430869, onlineIssueDateStr=2026-10-22, onlineJustAcceptDate=null, onlineJustAcceptDateStr=null, onlineFirstDate=null, onlineFirstDateStr=null, sourceXml=null, magXml=null, createTime=1792635430869, creator=13701087609, updateTime=1792635430869, updator=13701087609, issue=Issue{id=1319971875086783028, tenantId=1146029695717560320, journalId=1263187385517883426, year='2024', volume='52', issue='3', pageStart='737', pageEnd='1170', issueExtLink='null', onlineDate='null', pubDate='1710864000000', pubDateStr='2024-03-20', beforeIssueId=null, nextIssueId=null, price=null, status=1, issueComplete=1, articleOrder=1, issueType=-1, specialIssue=null, createTime=1792635418912, creator='13701087609', updateTime=1792641878851, updator='13701087609', preIssue=null, nextIssue=null, articleTotal=null, ext={EN=IssueExt(id=1319998970110264006, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319971875086783028, language=EN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=), CN=IssueExt(id=1319998970110264007, tenantId=1146029695717560320, journalId=1263187385517883426, issueId=1319971875086783028, language=CN, specialIssueTitle=, coverIllustrator=null, specialIssueEditor=, specialIssueAbout=)}, issueFiles=null, downloadFileDto=null}, startPage=755, endPage=764, ext={EN=ArticleExt(id=1319971925422616715, articleId=1319971925238067338, tenantId=1146029695717560320, journalId=1263187385517883426, language=EN, title=Effect of Ce Doping Concentration on Scintillation Performance of Ce,Ca:Lu3Al5O12 Ceramics, columnId=1319726165087077079, journalTitle=Journal of the Chinese Ceramic Society, columnName=Research Article, runingTitle=null, highlight=null, articleAbstract=
Introduction

Lutetium aluminum garnet (Lu3Al5O12, LuAG) is investigated as a classical scintillation material. LuAG can be fabricated in the form of single crystals, optical ceramics, thin films and other morphologies to meet different scintillation application demands. Cerium-doped LuAG (Ce:LuAG) ceramics can be used as a promising candidate for detection material in shashlik calorimeter for high-energy physics (HEP) experiments due to their high density, fast decay, efficient scintillation and relatively low cost. For HEP experiments with a high event rate, however, a slow scintillation component of Ce:LuAG ceramics leads to a pileup effect that needs to be diminished as much as possible. Divalent, optically inactive, Ca2+ co-doping is an effective strategy for suppressing slow scintillation component according to the defect engineering theory. In addition, the coprecipitated nano-powder can be also used as a raw material of ceramics, and improving the consistency of structure, composition and luminescence within the ceramics is also an important strategy to optimize the performance of Ce:LuAG scintillation ceramics. In this paper, Ce,Ca:LuAG ceramics with different Ce concentrations were prepared with the coprecipitation nano-powders. The effect of activator ion concentration on the decay behavior, light yield (LY) at different shaping times and afterglow intensity of Ce,Ca:LuAG ceramics were investigated.

Methods

A series of Ce,Ca:LuAG ceramics with the chemical composition of (CexCa0.001 5Lu0.998 5-x%)3Al5O12; x=0.1, 0.2, 0.3, 0.4, 0.5 were prepared with coprecipitated nano-powders through vacuum pre-sintering and hot isostatic pressed (HIP) post-treatment. In the process of nano-powder preparation, high purity Lu2O3 (99.995%), CeO2 (99.999%), and CaCO3 powders were dissolved in nitric acid solution, and Al(NO3)3·9H2O (AR) powders were dissolved in deionized water to obtain various nitrate solutions. The metal nitrate solutions were mixed and further diluted to a specific concentration. Ammonium hydrogen carbonate (AHC, 99%) was dissolved in de-ionized water as a precipitant solution, and ammonium sulfate (99%) was added into the precipitant solution as a dispersant. The mixed metal nitrate solution was dripped into the AHC solution under mild agitation at room temperature (RT). The resulting suspension was aged for 1 h and then washed with deionized water and ethanol. The precursor was dried, sieved and calcined to obtain Ce,Ca:LuAG nano-powders with a pure garnet phase. The powders were uniaxially dry-pressed into pellets at 20 MPa and then cold-isostatically pressed at 250 MPa. The green bodies were vacuum pre-sintered at 1 825 ℃ for 10 h, and then HIP in argon atmosphere under 176 MPa at 1 600 ℃ for 3 h. The fabricated Ce,Ca:LuAG ceramics were annealed in air at 1 450 ℃ for 10 h to remove oxygen vacancies introduced via sintering in a reducing atmosphere. The final Ce,Ca:LuAG ceramics were polished on the both sides to the thickness of 1 mm for the coming characterization.

Results and discussion

The XRD patterns of all the ceramic samples are in reasonable agreement with the standard XRD patterns of LuAG (PDF 73-1368), indicating that the main phase of the prepared ceramics is a LuAG garnet phase. The lattice parameters of Ce,Ca:LuAG ceramics with different Ce concentrations increase gradually with increasing doping concentration. The presence of Ce3+ can act as a sintering aid to accelerate the migration of grain boundaries during sintering of garnet ceramics and increase the average grain size. The absorption spectra of Ce,Ca:LuAG ceramics indicate that the amplitudes of 4f→5d1 transition at 447 nm and the 4f→5d2 transition at 345 nm of Ce3+ increase with the starting content of Ce3+ that evidences its entering into the garnet lattice. An intense absorption below 350 nm is due to the charge transfer absorption band induced by Ce4+ in the garnet lattice. The photoluminescence decay curves of the 5d1→4f emission of Ce3+ (510 nm) under the 452 nm excitation show that the fast component intensity I1 of all Ce,Ca:LuAG ceramics is > 95%. The main decay time shows an acceleration at the Ce concentration of > 0.3% because the formation of closely spaced (Ce4+—Ca2+) pairs can increase with the increase of Ce concentration. The scintillation decay under γ-excitation slightly slows down with increasing Ce concentration, since the proportion of induced Ce4+ decreases with increasing total Ce concentration, and the competition in accelerating scintillation process becomes progressively weaker. The X-ray excited luminescence (XEL) intensity of the Ce,Ca:LuAG ceramics firstly increases and then decreases with the Ce concentration, reaching the maximum value as x=0.3. The integral scintillation efficiency of Ce,Ca:LuAG ceramics is 146%-190% of a BGO crystal. The variation of the LY and the integral scintillation efficiency obtained from XEL have a similar pattern, i.e., increasing and then decreasing with the increase of Ce concentration. The optimum energy resolution (ER) is obtained as x=0.3. The normalized afterglow intensity after continuous X-ray irradiation monotonically decreases with the Ce concentration due to the more intense competition ability of cerium centers for charge carrier capture.

Conclusions

Ce,Ca:LuAG scintillation ceramics with different Ce concentrations were prepared with coprecipitation nano-powders via vacuum pre-sintering and HIP post-treatment. A small amount of Al-rich secondary phase existed in the ceramics due to the loss of lutetium during coprecipitation and washing, which could be avoided by component design in the future ceramic preparation. At the Ce concentration of 0.3%, Ce,Ca:LuAG ceramic had the optimum XEL integral efficiency, LY and ER. This study demonstrated that Ce doping concentration had a certain effect on the PL decay, scintillation decay and afterglow of Ce,Ca:LuAG ceramics, providing a guidance for the subsequent selection of doping concentration in practical applications.

, authors=Danyang ZHU1, 2, Jinling CAI1, 3, Alena BEITLEROVA4, Romana KUCERKOVA4, Weerapong CHEWPRADITKUL5, Martin NIKL4, Jiang LI1, 2, authorsList=Danyang ZHU, Jinling CAI, Alena BEITLEROVA, Romana KUCERKOVA, Weerapong CHEWPRADITKUL, Martin NIKL, Jiang LI, authorCompany=null, correspAuthors=Jiang LI, authorNote=

ZHU Danyang (1997-), female, Doctorial candidate. E-mail:

, correspAuthorsNote=
LI Jiang (1977-), male, Ph.D., Professor. E-mail:
, copyrightStatement=null, copyrightOwner=null, extLink=null, articleAbsUrl=null, sourceXml=null, magXml=null, pdfUrl=null, pdf=null, pdfFileSize=null, pdfExtLink=null, richHtmlUrl=null, mobilePdfUrl=null, reviewReport=null, pdfFirstPage=null, abstractGraph=null, abstractGraphContent=null, abstractVideo=null, citation=null, cebUrl=null, magXmlContent=null, mapNumber=null, fund=null), CN=ArticleExt(id=1319971925766549644, articleId=1319971925238067338, tenantId=1146029695717560320, journalId=1263187385517883426, language=CN, title=Ce掺杂浓度对Ce,Ca:Lu3Al5O12陶瓷闪烁性能的影响, columnId=1263922770220560512, journalTitle=硅酸盐学报, columnName=研究论文, runingTitle=null, highlight=null, articleAbstract=

以共沉淀纳米粉体为原料,制备不同Ce掺杂浓度的x%(摩尔分数)Ce,0.15%Ca:Lu3Al5O12(Ce, Ca:LuAG,x=0.1~0.5)闪烁陶瓷。在分析了Ce,Ca:LuAG陶瓷的相组成和微观结构的基础上,研究了其闪烁特性与Ce浓度的关系,包括X射线激发发射光谱、光致发光衰减、闪烁衰减、光产额及快分量、余辉。当Ce浓度超过0.3%时,光致发光衰减的加速证实了浓度猝灭的发生。Ce,Ca:LuAG陶瓷的X射线激发发射强度和光产额在Ce浓度为0.3%时达到最大值。随着Ce浓度的增加,陶瓷的余辉水平逐渐降低。最后讨论了Ce,Ca:LuAG闪烁陶瓷的制备和性能优化的策略。

, authors=朱丹阳1, 2, 蔡金伶1, 3, Alena BEITLEROVA4, Romana KUCERKOVA4, Weerapong CHEWPRADITKUL5, Martin NIKL4, 李江1, 2, authorsList=朱丹阳, 蔡金伶, Alena BEITLEROVA, Romana KUCERKOVA, Weerapong CHEWPRADITKUL, Martin NIKL, 李江, authorCompany=null, correspAuthors=李江, authorNote=

朱丹阳(1997—),女,博士研究生。

, correspAuthorsNote=
李江(1977—),男,博士,研究员。
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Ce掺杂浓度对Ce,Ca:Lu3Al5O12陶瓷闪烁性能的影响
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朱丹阳 1, 2 , 蔡金伶 1, 3 , Alena BEITLEROVA 4 , Romana KUCERKOVA 4 , Weerapong CHEWPRADITKUL 5 , Martin NIKL 4 , 李江 1, 2
硅酸盐学报 | 研究论文 2024,52(3): 755-764
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硅酸盐学报 |研究论文 2024 , 52 (3) : 755 -764
Ce掺杂浓度对Ce,Ca:Lu3Al5O12陶瓷闪烁性能的影响
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朱丹阳1, 2 , 蔡金伶1, 3, Alena BEITLEROVA4, Romana KUCERKOVA4, Weerapong CHEWPRADITKUL5, Martin NIKL4, 李江1, 2
作者信息
  • 1.中国科学院上海硅酸盐研究所,上海 201899,中国
  • 2.中国科学院大学,北京 100049,中国
  • 3.上海大学,上海 200072,中国
  • 4.捷克科学院物理研究所,布拉格 16200,捷克
  • 5.泰国国王科技大学,曼谷 10140,泰国
通讯作者:
李江(1977—),男,博士,研究员。
作者简介:

朱丹阳(1997—),女,博士研究生。

Effect of Ce Doping Concentration on Scintillation Performance of Ce,Ca:Lu3Al5O12 Ceramics
Danyang ZHU1, 2 , Jinling CAI1, 3, Alena BEITLEROVA4, Romana KUCERKOVA4, Weerapong CHEWPRADITKUL5, Martin NIKL4, Jiang LI1, 2
Affiliations
  • 1.Transparent Ceramics Research Center, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201899, China
  • 2.Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3.School of Materials Science and Engineering, Shanghai University, Shanghai 200072, China
  • 4.Institute of Physics of the Czech Academy of Sciences, Prague 16200, Czech Republic
  • 5King Mongkut's University of Technology Thonburi, Bangkok 10140, Thailand
  • Corresponding Author:
    LI Jiang (1977-), male, Ph.D., Professor. E-mail:

    ZHU Danyang (1997-), female, Doctorial candidate. E-mail:

出版时间: 2024-03-20 doi: 10.14062/j.issn.0454-5648.20230675
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以共沉淀纳米粉体为原料,制备不同Ce掺杂浓度的x%(摩尔分数)Ce,0.15%Ca:Lu3Al5O12(Ce, Ca:LuAG,x=0.1~0.5)闪烁陶瓷。在分析了Ce,Ca:LuAG陶瓷的相组成和微观结构的基础上,研究了其闪烁特性与Ce浓度的关系,包括X射线激发发射光谱、光致发光衰减、闪烁衰减、光产额及快分量、余辉。当Ce浓度超过0.3%时,光致发光衰减的加速证实了浓度猝灭的发生。Ce,Ca:LuAG陶瓷的X射线激发发射强度和光产额在Ce浓度为0.3%时达到最大值。随着Ce浓度的增加,陶瓷的余辉水平逐渐降低。最后讨论了Ce,Ca:LuAG闪烁陶瓷的制备和性能优化的策略。

铈  /  钙  /  镥铝石榴石陶瓷  /  闪烁性能  /  共沉淀法
Introduction

Lutetium aluminum garnet (Lu3Al5O12, LuAG) is investigated as a classical scintillation material. LuAG can be fabricated in the form of single crystals, optical ceramics, thin films and other morphologies to meet different scintillation application demands. Cerium-doped LuAG (Ce:LuAG) ceramics can be used as a promising candidate for detection material in shashlik calorimeter for high-energy physics (HEP) experiments due to their high density, fast decay, efficient scintillation and relatively low cost. For HEP experiments with a high event rate, however, a slow scintillation component of Ce:LuAG ceramics leads to a pileup effect that needs to be diminished as much as possible. Divalent, optically inactive, Ca2+ co-doping is an effective strategy for suppressing slow scintillation component according to the defect engineering theory. In addition, the coprecipitated nano-powder can be also used as a raw material of ceramics, and improving the consistency of structure, composition and luminescence within the ceramics is also an important strategy to optimize the performance of Ce:LuAG scintillation ceramics. In this paper, Ce,Ca:LuAG ceramics with different Ce concentrations were prepared with the coprecipitation nano-powders. The effect of activator ion concentration on the decay behavior, light yield (LY) at different shaping times and afterglow intensity of Ce,Ca:LuAG ceramics were investigated.

Methods

A series of Ce,Ca:LuAG ceramics with the chemical composition of (CexCa0.001 5Lu0.998 5-x%)3Al5O12; x=0.1, 0.2, 0.3, 0.4, 0.5 were prepared with coprecipitated nano-powders through vacuum pre-sintering and hot isostatic pressed (HIP) post-treatment. In the process of nano-powder preparation, high purity Lu2O3 (99.995%), CeO2 (99.999%), and CaCO3 powders were dissolved in nitric acid solution, and Al(NO3)3·9H2O (AR) powders were dissolved in deionized water to obtain various nitrate solutions. The metal nitrate solutions were mixed and further diluted to a specific concentration. Ammonium hydrogen carbonate (AHC, 99%) was dissolved in de-ionized water as a precipitant solution, and ammonium sulfate (99%) was added into the precipitant solution as a dispersant. The mixed metal nitrate solution was dripped into the AHC solution under mild agitation at room temperature (RT). The resulting suspension was aged for 1 h and then washed with deionized water and ethanol. The precursor was dried, sieved and calcined to obtain Ce,Ca:LuAG nano-powders with a pure garnet phase. The powders were uniaxially dry-pressed into pellets at 20 MPa and then cold-isostatically pressed at 250 MPa. The green bodies were vacuum pre-sintered at 1 825 ℃ for 10 h, and then HIP in argon atmosphere under 176 MPa at 1 600 ℃ for 3 h. The fabricated Ce,Ca:LuAG ceramics were annealed in air at 1 450 ℃ for 10 h to remove oxygen vacancies introduced via sintering in a reducing atmosphere. The final Ce,Ca:LuAG ceramics were polished on the both sides to the thickness of 1 mm for the coming characterization.

Results and discussion

The XRD patterns of all the ceramic samples are in reasonable agreement with the standard XRD patterns of LuAG (PDF 73-1368), indicating that the main phase of the prepared ceramics is a LuAG garnet phase. The lattice parameters of Ce,Ca:LuAG ceramics with different Ce concentrations increase gradually with increasing doping concentration. The presence of Ce3+ can act as a sintering aid to accelerate the migration of grain boundaries during sintering of garnet ceramics and increase the average grain size. The absorption spectra of Ce,Ca:LuAG ceramics indicate that the amplitudes of 4f→5d1 transition at 447 nm and the 4f→5d2 transition at 345 nm of Ce3+ increase with the starting content of Ce3+ that evidences its entering into the garnet lattice. An intense absorption below 350 nm is due to the charge transfer absorption band induced by Ce4+ in the garnet lattice. The photoluminescence decay curves of the 5d1→4f emission of Ce3+ (510 nm) under the 452 nm excitation show that the fast component intensity I1 of all Ce,Ca:LuAG ceramics is > 95%. The main decay time shows an acceleration at the Ce concentration of > 0.3% because the formation of closely spaced (Ce4+—Ca2+) pairs can increase with the increase of Ce concentration. The scintillation decay under γ-excitation slightly slows down with increasing Ce concentration, since the proportion of induced Ce4+ decreases with increasing total Ce concentration, and the competition in accelerating scintillation process becomes progressively weaker. The X-ray excited luminescence (XEL) intensity of the Ce,Ca:LuAG ceramics firstly increases and then decreases with the Ce concentration, reaching the maximum value as x=0.3. The integral scintillation efficiency of Ce,Ca:LuAG ceramics is 146%-190% of a BGO crystal. The variation of the LY and the integral scintillation efficiency obtained from XEL have a similar pattern, i.e., increasing and then decreasing with the increase of Ce concentration. The optimum energy resolution (ER) is obtained as x=0.3. The normalized afterglow intensity after continuous X-ray irradiation monotonically decreases with the Ce concentration due to the more intense competition ability of cerium centers for charge carrier capture.

Conclusions

Ce,Ca:LuAG scintillation ceramics with different Ce concentrations were prepared with coprecipitation nano-powders via vacuum pre-sintering and HIP post-treatment. A small amount of Al-rich secondary phase existed in the ceramics due to the loss of lutetium during coprecipitation and washing, which could be avoided by component design in the future ceramic preparation. At the Ce concentration of 0.3%, Ce,Ca:LuAG ceramic had the optimum XEL integral efficiency, LY and ER. This study demonstrated that Ce doping concentration had a certain effect on the PL decay, scintillation decay and afterglow of Ce,Ca:LuAG ceramics, providing a guidance for the subsequent selection of doping concentration in practical applications.

cerium  /  calcium  /  lutetium aluminum garnet ceramics  /  scintillation performance  /  coprecipitation method
朱丹阳, 蔡金伶, Alena BEITLEROVA, Romana KUCERKOVA, Weerapong CHEWPRADITKUL, Martin NIKL, 李江. Ce掺杂浓度对Ce,Ca:Lu3Al5O12陶瓷闪烁性能的影响. 硅酸盐学报, 2024 , 52 (3) : 755 -764 . DOI: 10.14062/j.issn.0454-5648.20230675
Danyang ZHU, Jinling CAI, Alena BEITLEROVA, Romana KUCERKOVA, Weerapong CHEWPRADITKUL, Martin NIKL, Jiang LI. Effect of Ce Doping Concentration on Scintillation Performance of Ce,Ca:Lu3Al5O12 Ceramics[J]. Journal of the Chinese Ceramic Society, 2024 , 52 (3) : 755 -764 . DOI: 10.14062/j.issn.0454-5648.20230675
  • 中国科学院国际合作计划项目(121631KYSB20200039)
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doi: 10.14062/j.issn.0454-5648.20230675
  • 接收时间:2023-09-01
  • 首发时间:2026-10-22
  • 出版时间:2024-03-20
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  • 收稿日期:2023-09-01
  • 修回日期:2023-09-25
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中国科学院国际合作计划项目(121631KYSB20200039)
作者信息
    1.中国科学院上海硅酸盐研究所,上海 201899,中国
    2.中国科学院大学,北京 100049,中国
    3.上海大学,上海 200072,中国
    4.捷克科学院物理研究所,布拉格 16200,捷克
    5.泰国国王科技大学,曼谷 10140,泰国

通讯作者:

李江(1977—),男,博士,研究员。
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2种不同金属材料的力学参数
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鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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