Dissimilar behavior of YAG:Ce and LuAG:Ce scintillator garnets regarding Li+ co-doping
Using a combination of experimental methods, the substitution tendencies of Li + and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce. The studies were performed on polycrystalline samples prepared by solid phase reactions...
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creator | Derdzyan, M. V Hovhannesyan, K. L Yeganyan, A. V Sargsyan, R. V Novikov, A Petrosyan, A. G Dujardin, C |
description | Using a combination of experimental methods, the substitution tendencies of Li
+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce. The studies were performed on polycrystalline samples prepared by solid phase reactions as well as in single crystals grown by the vertical Bridgman method. The results show that Li
+
in LuAG:Ce, Li is localized mainly at Lu
3+
sites with charge compensation brought about by Ce
3+
→ Ce
4+
conversion and creation of anion vacancies. Surprisingly, unlike LuAG:Ce, Li, no evidence for Li
+
substitution at Y
3+
sites and conversion of Ce
3+
to Ce
4+
has been obtained in YAG:Ce, Li. It suggests that Li
+
goes mainly to interstitial positions and does not interact with Ce
3+
. From an application point of view, Li
+
co-doping of YAG:Ce is not efficient to improve the scintillationdecay parameters, however, it is efficient to reduce the amount of anion vacancies in both YAG and YAG:Ce.
Using a combination of experimental methods, the substitution tendencies of Li
+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce. |
doi_str_mv | 10.1039/c7ce02194a |
format | Article |
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+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce. The studies were performed on polycrystalline samples prepared by solid phase reactions as well as in single crystals grown by the vertical Bridgman method. The results show that Li
+
in LuAG:Ce, Li is localized mainly at Lu
3+
sites with charge compensation brought about by Ce
3+
→ Ce
4+
conversion and creation of anion vacancies. Surprisingly, unlike LuAG:Ce, Li, no evidence for Li
+
substitution at Y
3+
sites and conversion of Ce
3+
to Ce
4+
has been obtained in YAG:Ce, Li. It suggests that Li
+
goes mainly to interstitial positions and does not interact with Ce
3+
. From an application point of view, Li
+
co-doping of YAG:Ce is not efficient to improve the scintillationdecay parameters, however, it is efficient to reduce the amount of anion vacancies in both YAG and YAG:Ce.
Using a combination of experimental methods, the substitution tendencies of Li
+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce.</description><identifier>ISSN: 1466-8033</identifier><identifier>EISSN: 1466-8033</identifier><identifier>DOI: 10.1039/c7ce02194a</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Anions ; Bridgman method ; Cerium ; Chemical Sciences ; Compensation ; Conversion ; Crystal growth ; Doping ; Engineering Sciences ; Garnets ; Physics ; Scintillation counters ; Single crystals ; Substitutes ; Vacancies ; Yttrium-aluminum garnet</subject><ispartof>CrystEngComm, 2018, Vol.2 (11), p.152-1526</ispartof><rights>Copyright Royal Society of Chemistry 2018</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c443t-1e12fb07fa2448fe20a51081a89c7206bb045230c8982bea807bc1b05f14c1b63</citedby><cites>FETCH-LOGICAL-c443t-1e12fb07fa2448fe20a51081a89c7206bb045230c8982bea807bc1b05f14c1b63</cites><orcidid>0000-0002-0205-9837</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,4010,27900,27901,27902</link.rule.ids><backlink>$$Uhttps://hal.science/hal-02287417$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Derdzyan, M. V</creatorcontrib><creatorcontrib>Hovhannesyan, K. L</creatorcontrib><creatorcontrib>Yeganyan, A. V</creatorcontrib><creatorcontrib>Sargsyan, R. V</creatorcontrib><creatorcontrib>Novikov, A</creatorcontrib><creatorcontrib>Petrosyan, A. G</creatorcontrib><creatorcontrib>Dujardin, C</creatorcontrib><title>Dissimilar behavior of YAG:Ce and LuAG:Ce scintillator garnets regarding Li+ co-doping</title><title>CrystEngComm</title><description>Using a combination of experimental methods, the substitution tendencies of Li
+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce. The studies were performed on polycrystalline samples prepared by solid phase reactions as well as in single crystals grown by the vertical Bridgman method. The results show that Li
+
in LuAG:Ce, Li is localized mainly at Lu
3+
sites with charge compensation brought about by Ce
3+
→ Ce
4+
conversion and creation of anion vacancies. Surprisingly, unlike LuAG:Ce, Li, no evidence for Li
+
substitution at Y
3+
sites and conversion of Ce
3+
to Ce
4+
has been obtained in YAG:Ce, Li. It suggests that Li
+
goes mainly to interstitial positions and does not interact with Ce
3+
. From an application point of view, Li
+
co-doping of YAG:Ce is not efficient to improve the scintillationdecay parameters, however, it is efficient to reduce the amount of anion vacancies in both YAG and YAG:Ce.
Using a combination of experimental methods, the substitution tendencies of Li
+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce.</description><subject>Anions</subject><subject>Bridgman method</subject><subject>Cerium</subject><subject>Chemical Sciences</subject><subject>Compensation</subject><subject>Conversion</subject><subject>Crystal growth</subject><subject>Doping</subject><subject>Engineering Sciences</subject><subject>Garnets</subject><subject>Physics</subject><subject>Scintillation counters</subject><subject>Single crystals</subject><subject>Substitutes</subject><subject>Vacancies</subject><subject>Yttrium-aluminum garnet</subject><issn>1466-8033</issn><issn>1466-8033</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNp90c9LwzAUB_AiCs7pxbtQ8aRSfS_J-sNbqdMJBS8qeAppmm4ZXVuTbuB_b2ZlevL0vi98eDxePO8U4QaBJrcykgoIJkzseSNkYRjEQOn-n3zoHVm7BECGCCPv7V5bq1e6FsYv1EJsdGv8tvLf08e7TPmiKf18PWQrddPruha9I3NhGtVb3yiXSt3M_Vxf-7INyrZz3bF3UInaqpOfOvZeH6Yv2SzInx-fsjQPJGO0D1AhqQqIKkEYiytFQEwQYhRxIiMCYVEAmxAKMk5iUigRQ1RILGBSIXM1pGPvcpi7EDXvjF4J88lbofkszfn2DQiJI4bRBp29GGxn2o-1sj1ftmvTuPU4AaRIQwTi1NWgpGmtNarajUXg2xvzLMqm3zdOHT4fsLFy537_gHdl5czZf4Z-ATglgK0</recordid><startdate>2018</startdate><enddate>2018</enddate><creator>Derdzyan, M. V</creator><creator>Hovhannesyan, K. L</creator><creator>Yeganyan, A. V</creator><creator>Sargsyan, R. V</creator><creator>Novikov, A</creator><creator>Petrosyan, A. G</creator><creator>Dujardin, C</creator><general>Royal Society of Chemistry</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>1XC</scope><scope>VOOES</scope><orcidid>https://orcid.org/0000-0002-0205-9837</orcidid></search><sort><creationdate>2018</creationdate><title>Dissimilar behavior of YAG:Ce and LuAG:Ce scintillator garnets regarding Li+ co-doping</title><author>Derdzyan, M. V ; Hovhannesyan, K. L ; Yeganyan, A. V ; Sargsyan, R. V ; Novikov, A ; Petrosyan, A. G ; Dujardin, C</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c443t-1e12fb07fa2448fe20a51081a89c7206bb045230c8982bea807bc1b05f14c1b63</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Anions</topic><topic>Bridgman method</topic><topic>Cerium</topic><topic>Chemical Sciences</topic><topic>Compensation</topic><topic>Conversion</topic><topic>Crystal growth</topic><topic>Doping</topic><topic>Engineering Sciences</topic><topic>Garnets</topic><topic>Physics</topic><topic>Scintillation counters</topic><topic>Single crystals</topic><topic>Substitutes</topic><topic>Vacancies</topic><topic>Yttrium-aluminum garnet</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Derdzyan, M. V</creatorcontrib><creatorcontrib>Hovhannesyan, K. L</creatorcontrib><creatorcontrib>Yeganyan, A. V</creatorcontrib><creatorcontrib>Sargsyan, R. V</creatorcontrib><creatorcontrib>Novikov, A</creatorcontrib><creatorcontrib>Petrosyan, A. G</creatorcontrib><creatorcontrib>Dujardin, C</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><jtitle>CrystEngComm</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Derdzyan, M. V</au><au>Hovhannesyan, K. L</au><au>Yeganyan, A. V</au><au>Sargsyan, R. V</au><au>Novikov, A</au><au>Petrosyan, A. G</au><au>Dujardin, C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dissimilar behavior of YAG:Ce and LuAG:Ce scintillator garnets regarding Li+ co-doping</atitle><jtitle>CrystEngComm</jtitle><date>2018</date><risdate>2018</risdate><volume>2</volume><issue>11</issue><spage>152</spage><epage>1526</epage><pages>152-1526</pages><issn>1466-8033</issn><eissn>1466-8033</eissn><abstract>Using a combination of experimental methods, the substitution tendencies of Li
+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce. The studies were performed on polycrystalline samples prepared by solid phase reactions as well as in single crystals grown by the vertical Bridgman method. The results show that Li
+
in LuAG:Ce, Li is localized mainly at Lu
3+
sites with charge compensation brought about by Ce
3+
→ Ce
4+
conversion and creation of anion vacancies. Surprisingly, unlike LuAG:Ce, Li, no evidence for Li
+
substitution at Y
3+
sites and conversion of Ce
3+
to Ce
4+
has been obtained in YAG:Ce, Li. It suggests that Li
+
goes mainly to interstitial positions and does not interact with Ce
3+
. From an application point of view, Li
+
co-doping of YAG:Ce is not efficient to improve the scintillationdecay parameters, however, it is efficient to reduce the amount of anion vacancies in both YAG and YAG:Ce.
Using a combination of experimental methods, the substitution tendencies of Li
+
and involved charge compensation mechanisms are determined and compared in two important similar scintillators, LuAG:Ce and YAG:Ce.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/c7ce02194a</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0002-0205-9837</orcidid><oa>free_for_read</oa></addata></record> |
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source | Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
subjects | Anions Bridgman method Cerium Chemical Sciences Compensation Conversion Crystal growth Doping Engineering Sciences Garnets Physics Scintillation counters Single crystals Substitutes Vacancies Yttrium-aluminum garnet |
title | Dissimilar behavior of YAG:Ce and LuAG:Ce scintillator garnets regarding Li+ co-doping |
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