人工晶体学报
人工晶體學報
인공정체학보
2009年
5期
1063-1067
,共5页
夏海平%张嗣春%王金浩%章践立
夏海平%張嗣春%王金浩%章踐立
하해평%장사춘%왕금호%장천립
近化学计量比LiNbO_3%助熔剂坩埚下降法%光谱
近化學計量比LiNbO_3%助鎔劑坩堝下降法%光譜
근화학계량비LiNbO_3%조용제감과하강법%광보
near-stoichiometric LiNbO_3 single crystal%flux bridgman method%spectra
以K_2O为助熔剂,应用坩埚下降法生长出了Co~(2+) 初始浓度为0.5 mol%,以及ZnO分别为3 mol%与6 mol%的单掺与双掺杂SLN晶体(分别用SLN0, SLN3, SLN6表示).测定了晶体上下部位的吸收与发射光谱.在晶体的吸收光谱中均可观察到520 nm,549 nm,612 nm,1447 nm四个吸收峰,表明Co~(2+)处于晶体的八面体场中.ZnO的掺入明显地改变了吸收峰的相对强度.在520 nm光的激发下,观察到776 nm的荧光发射,其荧光强度的相对强弱也与ZnO的掺杂量有明显的联系.从吸收边带估算出SLN0, SLN3, SLN6晶体中Li2O的含量分别为49.06 mol%,49.28 mol%, 49.10 mol%.ZnO的掺杂量对Co~(2+)在铌酸锂晶体中的浓度分布有很大的影响作用,当ZnO的掺入量为3 mol%时,明显地抑制了Co~(2+)在LiNbO_3晶体中的掺入,当ZnO掺杂量达到6 mol%时,抑制作用减弱.本文从Zn~(2+)在LiNbO_3中随浓度变化的分凝情况以及对Co~(2+)的排斥作用解释了Co~(2+)在晶体中的分布特性以及光谱的变化情况.
以K_2O為助鎔劑,應用坩堝下降法生長齣瞭Co~(2+) 初始濃度為0.5 mol%,以及ZnO分彆為3 mol%與6 mol%的單摻與雙摻雜SLN晶體(分彆用SLN0, SLN3, SLN6錶示).測定瞭晶體上下部位的吸收與髮射光譜.在晶體的吸收光譜中均可觀察到520 nm,549 nm,612 nm,1447 nm四箇吸收峰,錶明Co~(2+)處于晶體的八麵體場中.ZnO的摻入明顯地改變瞭吸收峰的相對彊度.在520 nm光的激髮下,觀察到776 nm的熒光髮射,其熒光彊度的相對彊弱也與ZnO的摻雜量有明顯的聯繫.從吸收邊帶估算齣SLN0, SLN3, SLN6晶體中Li2O的含量分彆為49.06 mol%,49.28 mol%, 49.10 mol%.ZnO的摻雜量對Co~(2+)在鈮痠鋰晶體中的濃度分佈有很大的影響作用,噹ZnO的摻入量為3 mol%時,明顯地抑製瞭Co~(2+)在LiNbO_3晶體中的摻入,噹ZnO摻雜量達到6 mol%時,抑製作用減弱.本文從Zn~(2+)在LiNbO_3中隨濃度變化的分凝情況以及對Co~(2+)的排斥作用解釋瞭Co~(2+)在晶體中的分佈特性以及光譜的變化情況.
이K_2O위조용제,응용감과하강법생장출료Co~(2+) 초시농도위0.5 mol%,이급ZnO분별위3 mol%여6 mol%적단참여쌍참잡SLN정체(분별용SLN0, SLN3, SLN6표시).측정료정체상하부위적흡수여발사광보.재정체적흡수광보중균가관찰도520 nm,549 nm,612 nm,1447 nm사개흡수봉,표명Co~(2+)처우정체적팔면체장중.ZnO적참입명현지개변료흡수봉적상대강도.재520 nm광적격발하,관찰도776 nm적형광발사,기형광강도적상대강약야여ZnO적참잡량유명현적련계.종흡수변대고산출SLN0, SLN3, SLN6정체중Li2O적함량분별위49.06 mol%,49.28 mol%, 49.10 mol%.ZnO적참잡량대Co~(2+)재니산리정체중적농도분포유흔대적영향작용,당ZnO적참입량위3 mol%시,명현지억제료Co~(2+)재LiNbO_3정체중적참입,당ZnO참잡량체도6 mol%시,억제작용감약.본문종Zn~(2+)재LiNbO_3중수농도변화적분응정황이급대Co~(2+)적배척작용해석료Co~(2+)재정체중적분포특성이급광보적변화정황.
Near-stoichiometric LiNbO_3 single crystals doped with 0.5mol% Co~(2+) and co-doped with Co~(2+) in 0.5mol% and Zn~(2+) in 3 mol% and 6 mol% (designated SLN0, SLN3, SLN6, respectively) in the raw compositions were grown by the Bridgman method under the conditions of taking K_2O as flux. The absorption spectra and emission spectra of upper and lower parts of crystals were measured. The absorption spectra showed the characteristic of Co~(2+) in octahedral co-ordination, and four absorption peaks at 520 nm, 549 nm, 612 nm, 1447 nm were observed in all the obtained crystals. However, the absorption intensity had an obvious change with the content of ZnO dopant. A sharp emission peak at 776 nm was observed under excitation of 520 nm light, and the emission intensity was also associated with the doping content of ZnO. The contents of Li2O were estimated from the absorption edge of SLN0, SLN3 and SLN6 to be 49.06 mol%,49.28 mol% and 49.1 mol%. The doping content of ZnO takes great effects on the distributing concentration of Co~(2+) in LiNbO_3 crystal. When 3% of ZnO in mole fraction is doped, the Co~(2+) are suppressed effectively to enter LiNbO_3 crystal sites, and the effect becomes weaker while the dopant of ZnO reaches to 6% mole fraction. The reasons for the concentration changes of Co~(2+) and spectra change can be interpreted by the suppressing effect of ZnO on the incorporation of Co~(2+) ions and the change of distribution coefficient of Zn~(2+) as its incorporating content.