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(Gd,Y,Ce)3(YxGa1−x)2GaAl2O12 (GYGAG:Ce) scintillation ceramics with different Y excess, where x = 0.005−0.08, were fabricated by the solid-state reaction method. The effects of stoichiometry on the phase composition, optical quality, and microstructure of GYGAG:Ce ceramics were analyzed. GYGAG:Ce ceramics have a pure garnet phase and obtain good in-line transmittance when x < 0.04, while more Y excess leads to the creation of the secondary phase. The change of x value influences the sintering behavior of the GYGAG:Ce ceramics: The excess of Y works as the self-sintering aid and significantly reduces the sintering temperature of ceramics. When x = 0.01–0.04, the X-ray excited luminescence (XEL) spectra and light yields of GYGAG:Ce ceramics are similar. The fast scintillation decay time and afterglow intensity of GYGAG:Ce ceramics show a slight decrease with increasing x value. Finally, additional 50–500 ppm MgO and 100–500 ppm CaO were introduced to the GYGAG:Ce ceramic with x = 0.04, and both were found to significantly increase the fast scintillation component and reduce the afterglow intensity by two orders of magnitude to 0.01% after X-ray cut-off.


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Compositional regulation of multi-component GYGAG:Ce scintillation ceramics: Self-sintering-aid effect and afterglow suppression

Show Author's information Danyang Zhua,bLexiang WuaAlena BeitlerovacRomana KucerkovacWeerapong ChewpraditkuldMartin NiklcJiang Lia,b( )
Transparent Ceramics Research Center, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201899, China
Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
Institute of Physics of the Czech Academy of Sciences, Prague 16200, Czech Republic
King Mongkut’s University of Technology Thonburi, Bangkok 10140, Thailand

Abstract

(Gd,Y,Ce)3(YxGa1−x)2GaAl2O12 (GYGAG:Ce) scintillation ceramics with different Y excess, where x = 0.005−0.08, were fabricated by the solid-state reaction method. The effects of stoichiometry on the phase composition, optical quality, and microstructure of GYGAG:Ce ceramics were analyzed. GYGAG:Ce ceramics have a pure garnet phase and obtain good in-line transmittance when x < 0.04, while more Y excess leads to the creation of the secondary phase. The change of x value influences the sintering behavior of the GYGAG:Ce ceramics: The excess of Y works as the self-sintering aid and significantly reduces the sintering temperature of ceramics. When x = 0.01–0.04, the X-ray excited luminescence (XEL) spectra and light yields of GYGAG:Ce ceramics are similar. The fast scintillation decay time and afterglow intensity of GYGAG:Ce ceramics show a slight decrease with increasing x value. Finally, additional 50–500 ppm MgO and 100–500 ppm CaO were introduced to the GYGAG:Ce ceramic with x = 0.04, and both were found to significantly increase the fast scintillation component and reduce the afterglow intensity by two orders of magnitude to 0.01% after X-ray cut-off.

Keywords: afterglow, GYGAG:Ce ceramics, multi-component garnet, compositional regulation

References(47)

[1]
Korzhik M, Abashev R, Fedorov A, et al. Towards effective indirect radioisotope energy converters with bright and radiation hard scintillators of (Gd,Y)3Al2Ga3O12 family. Nucl Eng Technol 2022, 54: 2579–2585.
[2]
Cherepy NJ, Kuntz JD, Seeley ZM, et al. Transparent ceramic scintillators for gamma spectroscopy and radiography. In: Proceedings of the SPIE 7805, Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XII, San Diego, California, USA, 2010: 69–73.
DOI
[3]
Zhu DY, Nikl M, Chewpraditkul W, et al. Development and prospects of garnet ceramic scintillators: A review. J Adv Ceram 2022, 11: 1825–1848.
[4]
Fu J, Feng SW, Guo YC, et al. Ce3+:Lu3Al5O12–Al2O3 optical nanoceramic scintillators elaborated via a low-temperature glass crystallization route. J Adv Ceram 2023, 12: 268–278.
[5]
Kim C, Lee W, Melis A, et al. A review of inorganic scintillation crystals for extreme environments. Crystals 2021, 11: 669.
[6]
Cherepy NJ, Seeley ZM, Payne SA, et al. Development of transparent ceramic Ce-doped gadolinium garnet gamma spectrometers. IEEE Trans Nucl Sci 2013, 60: 2330–2335.
[7]
Jarrell JT, Cherepy N, Seeley Z, et al. Radiation hardness of polycrystalline ceramic scintillators for radioisotope batteries. In: Proceedings of the SPIE 12241, Hard X-Ray, Gamma-Ray, and Neutron Detector Physics XXIV, San Diego, California, USA, 2022: 156–165.
DOI
[8]
Chewpraditkul W, Pattanaboonmee N, Sakthong O, et al. Scintillation characteristics and temperature quenching of radio- and photoluminescence of Mg2+-codoped (Lu, Gd)3Al2.4Ga2.6O12:Ce garnet crystals. Opt Mater 2021, 121: 111595.
[9]
You Q, Lin H, Hong RJ, et al. Structural and scintillation properties of Ce3+:Gd3Al3Ga2O12 translucent ceramics prepared by one-step sintering. Materials 2023, 16: 3373.
[10]
Korzhik M, Retivov V, Bondarau A, et al. Role of the dilution of the Gd sublattice in forming the scintillation properties of quaternary (Gd,Lu)3Al2Ga3O12:Ce ceramics. Crystals 2022, 12: 1196.
[11]
Martinazzoli L, Nargelas S, Boháček P, et al. Compositional engineering of multicomponent garnet scintillators: Towards an ultra-accelerated scintillation response. Mater Adv 2022, 3: 6842–6852.
[12]
Nargelas S, Talochka Y, Vaitkevičius A, et al. Influence of matrix composition and its fluctuations on excitation relaxation and emission spectrum of Ce ions in (GdxY1–x)3Al2Ga3O12:Ce scintillators. J Lumin 2022, 242: 118590.
[13]
Kuznetsova D, Dubov V, Bondarev A, et al. Tailoring of the Gd–Y–Lu ratio in quintuple (Gd,Lu,Y)3Al2Ga3O12:Ce ceramics for better scintillation properties. J Appl Phys 2022, 132: 203104.
[14]
Zazubovich S, Laguta VV, Machek P, et al. Effect of Li+ co-doping on the luminescence and defects creation processes in Gd3(Ga,Al)5O12:Ce scintillation crystals. J Lumin 2022, 242: 118548.
[15]
Ogino H, Yoshikawa A, Nikl M, et al. Suppression of defect related host luminescence in LuAG single crystals. Phys Procedia 2009, 2: 191–205.
[16]
Ogino H, Yoshikawa A, Nikl M, et al. Growth and optical properties of Lu3(Ga,Al)5O12 single crystals for scintillator application. J Cryst Growth 2009, 311: 908–911.
[17]
Chen XP, Hu ZW, Dai JW, et al. Fabrication and optical properties of cerium doped Lu3Ga3Al2O12 scintillation ceramics. Opt Mater 2018, 85: 121–126.
[18]
Kamada K, Endo T, Tsutumi K, et al. Composition engineering in cerium-doped (Lu,Gd)3(Ga,Al)5O12 single-crystal scintillators. Cryst Growth Des 2011, 11: 4484–4490.
[19]
Fasoli M, Vedda A, Nikl M, et al. Band-gap engineering for removing shallow traps in rare-earth Lu3Al5O12 garnet scintillators using Ga3+ doping. Phys Rev B 2011, 84: 081102.
[20]
Retivov V, Dubov V, Kuznetsova D, et al. Gd3+ content optimization for mastering high light yield and fast GdxAl2Ga3O12:Ce3+ scintillation ceramics. J Rare Earths 2022, .
[21]
Li JG, Sakka Y. Recent progress in advanced optical materials based on gadolinium aluminate garnet (Gd3Al5O12). Sci Technol Adv Mater 2015, 16: 014902.
[22]
Ermakova LV, Dubov VV, Saifutyarov RR, et al. Influence of luminescent properties of powders on the fabrication of scintillation ceramics by stereolithography 3D printing. Ceramics 2023, 6: 43–57.
[23]
Karpyuk P, Shurkina A, Kuznetsova D, et al. Effect of sintering additives on the sintering and spectral-luminescent characteristics of quaternary GYAGG:Ce scintillation ceramics. J Electron Mater 2022, 51: 6481–6491.
[24]
Jarrell JT, Cherepy NJ, Seeley ZM, et al. Beta radiation hardness of GYGAG(Ce) transparent ceramic scintillators. IEEE Trans Nucl Sci 2022, 69: 938–941.
[25]
Chen XP, Hu ZW, Feng YG, et al. Luminescence and scintillation characteristics of cerium doped Gd2YGa3Al2O12 ceramics. Opt Mater 2019, 90: 20–25.
[26]
Chen XP, Liu X, Feng YG, et al. Microstructure evolution in two-step-sintering process toward transparent Ce:(Y, Gd)3(Ga,Al)5O12 scintillation ceramics. J Alloys Compd 2020, 846: 156377.
[27]
Seeley ZM, Cherepy NJ, Payne SA. Expanded phase stability of Gd-based garnet transparent ceramic scintillators. J Mater Res 2014, 29: 2332–2337.
[28]
Zhang JY, Luo ZH, Liu YF, et al. Cation-substitution induced stable GGAG:Ce3+ ceramics with improved optical and scintillation properties. J Eur Ceram Soc 2017, 37: 4925–4930.
[29]
Zhu DY, Chen XP, Beitlerova A, et al. Influence of calcium doping concentration on the performance of Ce,Ca:LuAG scintillation ceramics. J Eur Ceram Soc 2022, 42: 6075–6084.
[30]
Zhu DY, Qian K, Chen XP, et al. Fine-grained Ce,Y:SrHfO3 scintillation ceramics fabricated by hot isostatic pressing. J Inorg Mater 2021, 36: 1118.
[31]
Zhou GH, Wang ZJ, Zhou BZ, et al. Fabrication of transparent Y2Hf2O7 ceramics via vacuum sintering. Opt Mater 2013, 35: 774–777.
[32]
Hostaša J, Cova F, Piancastelli A, et al. Fabrication and luminescence of Ce-doped GGAG transparent ceramics, effect of sintering parameters and additives. Ceram Int 2019, 45: 23283–23288.
[33]
Chen XQ, Qin HM, Zhang Y, et al. Highly transparent ZrO2-doped (Ce,Gd)3Al3Ga2O12 ceramics prepared via oxygen sintering. J Eur Ceram Soc 2015, 35: 3879–3883.
[34]
Shen YQ, Shi Y, Feng XQ, et al. The harmful effects of sintering aids in Pr:LuAG optical ceramic scintillator. J Am Ceram Soc 2012, 95: 2130–2132.
[35]
Liu SP, Feng XQ, Nikl M, et al. Fabrication and scintillation performance of nonstoichiometric LuAG:Ce ceramics. J Am Ceram Soc 2015, 98: 510–514.
[36]
Hu ZW, Chen XP, Dai JW, et al. The influences of stoichiometry on the sintering behavior, optical and scintillation properties of Pr:LuAG ceramics. J Eur Ceram Soc 2018, 38: 4252–4259.
[37]
Hu C, Liu SP, Fasoli M, et al. ESR and TSL study of hole and electron traps in LuAG:Ce,Mg ceramic scintillator. Opt Mater 2015, 45: 252–257.
[38]
Chewpraditkul W, Pattanaboonmee N, Chewpraditkul W, et al. Optical and scintillation characteristics of Lu2Y(Al5–xGax)O12:Ce,Mg multicomponent garnet crystals. Opt Mater 2022, 134: 113186.
[39]
Dormenev V, Brinkmann KT, Kazlou D, et al. Scintillation properties of garnets and oxyorthosilicates with different dopants. IEEE Trans Nucl Sci 2023, 70: 1392–1397.
[40]
Cai JL, Zhu DY, Hu DJ, et al. Characterization of Ce,Ca:LuAG ceramic scintillators fabricated from co-precipitated powders. Opt Mater 2022, 133: 113051.
[41]
Liu SP, Feng XQ, Zhou ZW, et al. Effect of Mg2+ co-doping on the scintillation performance of LuAG:Ce ceramics. Phys Status Solidi RRL 2014, 8: 105–109.
[42]
Liu SP, Mares JA, Feng XQ, et al. Towards bright and fast Lu3Al5O12:Ce,Mg optical ceramics scintillators. Adv Opt Mater 2016, 4: 731–739.
[43]
Huang X, He J, Jiang YG, et al. Ultrafast GGAG:Ce X-ray scintillation ceramics with Ca2+ and Mg2+ co-dopants. Ceram Int 2022, 48: 23571–23577.
[44]
Dosovitskiy G, Dubov V, Karpyuk P, et al. Activator segregation and micro-luminescence properties in GAGG:Ce ceramics. J Lumin 2021, 236: 118140.
[45]
Korzhik M, Alenkov V, Buzanov O, et al. Engineering of a new single-crystal multi-ionic fast and high-light-yield scintillation material (Gd0.5–Y0.5)3Al2Ga3O12:Ce,Mg. CrystEngComm 2020, 22: 2502–2506.
[46]
Babin V, Boháček P, Jurek K, et al. Dependence of Ce3+-related photo and thermally stimulated luminescence characteristics on Mg2+ content in single crystals and epitaxial films of Gd3(Ga,Al)5O12:Ce,Mg. Opt Mater 2018, 83: 290–299.
[47]
Babin V, Herman P, Kucera M, et al. Effect of Mg2+ co-doping on the photo- and thermally stimulated luminescence of the (Lu,Gd)3(Ga,Al)5O12:Ce epitaxial films. J Lumin 2019, 215: 116608.
Publication history
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Publication history

Received: 18 June 2023
Revised: 27 July 2023
Accepted: 16 August 2023
Published: 25 October 2023
Issue date: October 2023

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© The Author(s) 2023.

Acknowledgements

This work was supported by the International Partnership Program of Chinese Academy of Sciences (Grant No. 121631KYSB20200039), the International Cooperation Project of Shanghai Science and Technology Commission (Grant No. 20520750200), the National Key R&D Program of China (Grant No. 2021YFE0104800), and the Key Research Project of the Frontier Science of the Chinese Academy of Sciences (Grant No. QYZDB-SSW-JSC022). Partial support of the Czech Ministry of Education, Youth and Sports under Project SOLID21 CZ.02.1. (Grant No. 01/0.0/0.0/16_019/0000760) and Czech Science Foundation project (Grant No. GA21-17731S) is acknowledged with thanks.

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