{"title":"LuAP:Ce中的电荷阱和发射动力学","authors":"J. Glodo, A. Wojtowicz","doi":"10.1117/12.435828","DOIUrl":null,"url":null,"abstract":"In this contribution we demonstrate the influence of shallow charge traps on emissions kinetics of LuAlO3:Ce3+ scintillator. Shallow traps through their interference with the recombination process not only introduce into the emission time profiles long components but also can change the rising and decaying parts of time profiles. The lifetime of excited Ce3+ ion in LuAP crystal is approximately 18 ns, while the excitation at 78 nm leads to the emission described by 21.5 and 1.22 ns decay and rise time constants, respectively. Furthermore, temperature dependence of time profile phase is observed. The analysis of emissions kinetics measured against temperature shows that observed features can be explained in terms of a trap described by the following parameters: E equals 0.142 eV and S equals 6.087 X 1010 s-1.","PeriodicalId":365405,"journal":{"name":"International Conference on Solid State Crystals","volume":"28 5-6","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2001-08-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Charge traps and emission kinetics in LuAP:Ce\",\"authors\":\"J. Glodo, A. Wojtowicz\",\"doi\":\"10.1117/12.435828\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this contribution we demonstrate the influence of shallow charge traps on emissions kinetics of LuAlO3:Ce3+ scintillator. Shallow traps through their interference with the recombination process not only introduce into the emission time profiles long components but also can change the rising and decaying parts of time profiles. The lifetime of excited Ce3+ ion in LuAP crystal is approximately 18 ns, while the excitation at 78 nm leads to the emission described by 21.5 and 1.22 ns decay and rise time constants, respectively. Furthermore, temperature dependence of time profile phase is observed. The analysis of emissions kinetics measured against temperature shows that observed features can be explained in terms of a trap described by the following parameters: E equals 0.142 eV and S equals 6.087 X 1010 s-1.\",\"PeriodicalId\":365405,\"journal\":{\"name\":\"International Conference on Solid State Crystals\",\"volume\":\"28 5-6\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2001-08-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Conference on Solid State Crystals\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1117/12.435828\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Conference on Solid State Crystals","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.435828","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
摘要
在这篇贡献中,我们证明了浅电荷陷阱对LuAlO3:Ce3+闪烁体发射动力学的影响。浅层陷阱通过对复合过程的干扰,不仅在发射时间谱中引入了长分量,而且改变了发射时间谱的上升和衰减部分。在LuAP晶体中,Ce3+离子的激发寿命约为18 ns,而在78 nm激发时,其衰变和上升时间常数分别为21.5 ns和1.22 ns。此外,还观察到时间剖面相位的温度依赖性。根据温度测量的发射动力学分析表明,所观察到的特征可以用以下参数描述的陷阱来解释:E等于0.142 eV, S等于6.087 X 1010 S -1。
In this contribution we demonstrate the influence of shallow charge traps on emissions kinetics of LuAlO3:Ce3+ scintillator. Shallow traps through their interference with the recombination process not only introduce into the emission time profiles long components but also can change the rising and decaying parts of time profiles. The lifetime of excited Ce3+ ion in LuAP crystal is approximately 18 ns, while the excitation at 78 nm leads to the emission described by 21.5 and 1.22 ns decay and rise time constants, respectively. Furthermore, temperature dependence of time profile phase is observed. The analysis of emissions kinetics measured against temperature shows that observed features can be explained in terms of a trap described by the following parameters: E equals 0.142 eV and S equals 6.087 X 1010 s-1.