辽宁石油化工大学学报
遼寧石油化工大學學報
료녕석유화공대학학보
JOURNAL OF LIAONING UNIVERSITY OF PETROLEUM & CHEMICAL TECHNOLOGY
2014年
1期
23-26
,共4页
王德%陈鹏%纪灵娴%黄玮%丛玉凤
王德%陳鵬%紀靈嫻%黃瑋%叢玉鳳
왕덕%진붕%기령한%황위%총옥봉
稀土%溶胶-凝胶法%硅酸盐%蓄能发光材料%发射光谱
稀土%溶膠-凝膠法%硅痠鹽%蓄能髮光材料%髮射光譜
희토%용효-응효법%규산염%축능발광재료%발사광보
Rare earth%Sol-gel method%Silicate%Energy storage luminescent materials%Emission spectrum
以正硅酸乙酯、CaO、Eu2 O3和Dy2 O3为原料,采用溶胶-凝胶法制备了硅酸盐蓄能发光材料CaSiO3:Eu2+,Dy3+,并利用X射线衍射、荧光光谱等分析手段研究了蓄能发光材料的晶格结构、光谱特性和影响材料发光性能的工艺因素。结果表明,灼烧温度对样品晶格结构及发光性能有重要影响。当温度低于1300℃时,样品晶格结构发育不完善,温度高于1400℃时,样品容易产生烧结现象。Eu2+作为发光中心,其浓度对样品发光性能有重要影响,当Eu2+掺杂的物质的量为0.005 mol时,样品发光强度最大,此时,样品的发射光谱是一个峰值位于544 nm的不对称宽带发射。
以正硅痠乙酯、CaO、Eu2 O3和Dy2 O3為原料,採用溶膠-凝膠法製備瞭硅痠鹽蓄能髮光材料CaSiO3:Eu2+,Dy3+,併利用X射線衍射、熒光光譜等分析手段研究瞭蓄能髮光材料的晶格結構、光譜特性和影響材料髮光性能的工藝因素。結果錶明,灼燒溫度對樣品晶格結構及髮光性能有重要影響。噹溫度低于1300℃時,樣品晶格結構髮育不完善,溫度高于1400℃時,樣品容易產生燒結現象。Eu2+作為髮光中心,其濃度對樣品髮光性能有重要影響,噹Eu2+摻雜的物質的量為0.005 mol時,樣品髮光彊度最大,此時,樣品的髮射光譜是一箇峰值位于544 nm的不對稱寬帶髮射。
이정규산을지、CaO、Eu2 O3화Dy2 O3위원료,채용용효-응효법제비료규산염축능발광재료CaSiO3:Eu2+,Dy3+,병이용X사선연사、형광광보등분석수단연구료축능발광재료적정격결구、광보특성화영향재료발광성능적공예인소。결과표명,작소온도대양품정격결구급발광성능유중요영향。당온도저우1300℃시,양품정격결구발육불완선,온도고우1400℃시,양품용역산생소결현상。Eu2+작위발광중심,기농도대양품발광성능유중요영향,당Eu2+참잡적물질적량위0.005 mol시,양품발광강도최대,차시,양품적발사광보시일개봉치위우544 nm적불대칭관대발사。
CaSiO3 :Eu2+ ,Dy3+ silicates storage luminescent materials were prepared by sol-gel method that use ethyl silicate , CaO ,Eu2 O3 ,Dy2 O3 as the starting materials . The lattice structure and spectroscopic properties of storage luminescent materials and the influencing factors on luminescence properties were studied by X-ray diffraction ,fluorescence spectrum and other analytical tools . The results indicate that the calcination temperature have great influence on lattice structure and luminescence properties of sample .When the temperature is below 1 300 ℃ ,crystal lattice structure of sample is imperfect . The temperature higher than 1 400 ℃ ,the sample is prone to produce sintering phenomenon .Eu2+ as luminescent centers and its concentration have great influence on luminescence properties of samples .When the Eu2+ concentration was 0 .005 mol ,the luminous intensity of sample reached the maximum .In this case ,the emission spectrum of the sample was an asymmetrical transmission that the peak located in 544 nm .