Crystal growth and scintillation properties of Ce doped (Gd,Y)AlO3 perovskite single crystals
Ce1%:(GdxY1‐x)AlO3 (x=0, 0.2, 0.4, 0.6, 0.8 and 1) crystals were grown by the μ‐PD method with RF heating system. All of the grown crystals show single perovskite phase. Ce3+ 4f‐5d emission is observed within 360‐400nm wavelength. Emission peak shifts to shorter wavelength with increasing Y concentr...
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Veröffentlicht in: | Physica status solidi. C 2012-12, Vol.9 (12), p.2263-2266 |
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description | Ce1%:(GdxY1‐x)AlO3 (x=0, 0.2, 0.4, 0.6, 0.8 and 1) crystals were grown by the μ‐PD method with RF heating system. All of the grown crystals show single perovskite phase. Ce3+ 4f‐5d emission is observed within 360‐400nm wavelength. Emission peak shifts to shorter wavelength with increasing Y concentration. In order to determine light yield, the energy spectra were collected under 662 keV γ‐ray excitation (137Cs source) and detection by an PMT R6451(Hamamatsu). The light yield was calculated by comparing to LYSO standard. The light yield of Ce1%:(GdxY1‐x)AlO3samples were increased with increasing Y concentration and Ce1%:Gd0.6Y0.4AlO3sample shows the highest light yield of 14,000 photon/MeV. Scintillation decay time was around 14.4 ns (16%) with slower decay component of.139 ns (84%) (© 2012 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) |
doi_str_mv | 10.1002/pssc.201200264 |
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All of the grown crystals show single perovskite phase. Ce3+ 4f‐5d emission is observed within 360‐400nm wavelength. Emission peak shifts to shorter wavelength with increasing Y concentration. In order to determine light yield, the energy spectra were collected under 662 keV γ‐ray excitation (137Cs source) and detection by an PMT R6451(Hamamatsu). The light yield was calculated by comparing to LYSO standard. The light yield of Ce1%:(GdxY1‐x)AlO3samples were increased with increasing Y concentration and Ce1%:Gd0.6Y0.4AlO3sample shows the highest light yield of 14,000 photon/MeV. Scintillation decay time was around 14.4 ns (16%) with slower decay component of.139 ns (84%) (© 2012 WILEY‐VCH Verlag GmbH & Co. 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Status Solidi C</addtitle><description>Ce1%:(GdxY1‐x)AlO3 (x=0, 0.2, 0.4, 0.6, 0.8 and 1) crystals were grown by the μ‐PD method with RF heating system. All of the grown crystals show single perovskite phase. Ce3+ 4f‐5d emission is observed within 360‐400nm wavelength. Emission peak shifts to shorter wavelength with increasing Y concentration. In order to determine light yield, the energy spectra were collected under 662 keV γ‐ray excitation (137Cs source) and detection by an PMT R6451(Hamamatsu). The light yield was calculated by comparing to LYSO standard. The light yield of Ce1%:(GdxY1‐x)AlO3samples were increased with increasing Y concentration and Ce1%:Gd0.6Y0.4AlO3sample shows the highest light yield of 14,000 photon/MeV. Scintillation decay time was around 14.4 ns (16%) with slower decay component of.139 ns (84%) (© 2012 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</description><subject>Crystals</subject><subject>micro-pulling method</subject><subject>scintillator</subject><subject>single crystal</subject><issn>1862-6351</issn><issn>1610-1642</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNo9UE1Lw0AQXUTBWr16XvCiYOp-JzmWoFWotlJFPMiyTTZ125jE3a21_94tkZ5mHvPezLwHwDlGA4wQuWmdywcEYRKAYAeghwVGERaMHIY-ESQSlONjcOLcEiHKERY98JHZrfOqggvbbPwnVHUBXW5qb6pKedPUsLVNq6032sGmhJmGRcAFvBwV1-9Xw2pCYRg3P25lvIbO1ItKw7xb6k7BURmKPvuvffB6d_uS3UfjyeghG44jQ2nMwl8kUQWZa1yglJVkjoRSOWdaE53kSYzUXPM44UgXGrNUEFwGh4whpTBPy5L2wUW3Nzz7vdbOy2WztnU4KTFlPA1eOQqstGNtTKW3srXmS9mtxEju8pO7_OQ-PzmdzbI9Ctqo0xrn9e9eq-xKipjGXL49jeR0SlhM0aN8pn-GFXWW</recordid><startdate>201212</startdate><enddate>201212</enddate><creator>Kamada, Kei</creator><creator>Endo, Takanori</creator><creator>Tsutsumi, Kousuke</creator><creator>Yoshikawa, Akira</creator><general>WILEY-VCH Verlag</general><general>WILEY‐VCH Verlag</general><general>Wiley Subscription Services, Inc</general><scope>BSCLL</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>201212</creationdate><title>Crystal growth and scintillation properties of Ce doped (Gd,Y)AlO3 perovskite single crystals</title><author>Kamada, Kei ; Endo, Takanori ; Tsutsumi, Kousuke ; Yoshikawa, Akira</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i3374-6328ad2be1d094f2b06aac54ee2e8c870abe57850ede149621f264440aa159ff3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Crystals</topic><topic>micro-pulling method</topic><topic>scintillator</topic><topic>single crystal</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kamada, Kei</creatorcontrib><creatorcontrib>Endo, Takanori</creatorcontrib><creatorcontrib>Tsutsumi, Kousuke</creatorcontrib><creatorcontrib>Yoshikawa, Akira</creatorcontrib><collection>Istex</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica status solidi. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kamada, Kei</au><au>Endo, Takanori</au><au>Tsutsumi, Kousuke</au><au>Yoshikawa, Akira</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Crystal growth and scintillation properties of Ce doped (Gd,Y)AlO3 perovskite single crystals</atitle><jtitle>Physica status solidi. C</jtitle><addtitle>Phys. Status Solidi C</addtitle><date>2012-12</date><risdate>2012</risdate><volume>9</volume><issue>12</issue><spage>2263</spage><epage>2266</epage><pages>2263-2266</pages><issn>1862-6351</issn><eissn>1610-1642</eissn><abstract>Ce1%:(GdxY1‐x)AlO3 (x=0, 0.2, 0.4, 0.6, 0.8 and 1) crystals were grown by the μ‐PD method with RF heating system. All of the grown crystals show single perovskite phase. Ce3+ 4f‐5d emission is observed within 360‐400nm wavelength. Emission peak shifts to shorter wavelength with increasing Y concentration. In order to determine light yield, the energy spectra were collected under 662 keV γ‐ray excitation (137Cs source) and detection by an PMT R6451(Hamamatsu). The light yield was calculated by comparing to LYSO standard. The light yield of Ce1%:(GdxY1‐x)AlO3samples were increased with increasing Y concentration and Ce1%:Gd0.6Y0.4AlO3sample shows the highest light yield of 14,000 photon/MeV. Scintillation decay time was around 14.4 ns (16%) with slower decay component of.139 ns (84%) (© 2012 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)</abstract><cop>Berlin</cop><pub>WILEY-VCH Verlag</pub><doi>10.1002/pssc.201200264</doi><tpages>4</tpages></addata></record> |
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title | Crystal growth and scintillation properties of Ce doped (Gd,Y)AlO3 perovskite single crystals |
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