新型激光晶體Nd:GSAG和Cr,Nd:GSAG的生長及光學(xué)性能研究
[Abstract]:High uniformity and large size laser crystals are the important basis for the development of all-solid-state high-power lasers, while space lasers need to develop high-efficiency laser crystals with anti-radiation properties. The coagulation coefficient of Nd3 in GSAG is about three times that of YAG, and the melting point is slightly lower than that of YAG. It is expected that the large size and high uniformity laser crystal element will be prepared, and it is similar to the structure and performance of Cr,Nd:GSGG with excellent radiation resistance. Therefore, Nd and Nd,Cr doped GSAG are selected as the research objects in this paper. Large size and high uniformity laser crystals and laser crystals with excellent radiation resistance are to be explored. The main contents and results are as follows: firstly, Nd:GSAG crystals with diameter 桅 30mm have been successfully grown by Czochralski method, the effective coagulation coefficients of Nd3 in GSAG have been measured, and the structural parameters have been obtained by Rietveld full-spectrum fitting. The absorption and luminescence of Nd:GSAG at room temperature are studied. The effective segregation coefficient of Nd3 at room temperature is 0.53, the strongest absorption peak is at 808.6nm, the absorption cross section is 3.44 脳 10-20cm2, the transition intensity parameter 惟 t (ttm2m2c2c2c2c2c2n) is 3.010 脳 10-20cm2n 2, the strongest emission peak is at 1060nm, the emission cross section of 1060nmmnm941.5nm is 6.32 脳 10-20cm2.77 脳 10-20cm2cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2.77 脳 10-20cm2, respectively. The lifetime of the corresponding laser upper level 4F3/2 is 258 渭 s. The 808nm CW semiconductor laser (LD) is used as the pump source to study the 1.06 渭 m laser performance of 2mm 脳 2mm 脳 6mm Nd:GSAG. The threshold value is 2.139 W, the slope efficiency is 8.9 W, the maximum output power is 0.462 W, and the optical-optical conversion efficiency is 5.12 W. In addition, the thermal diffusivity of Nd:GSAG crystal in the range of 297K-748K was measured. The thermal conductivity of Nd:GSAG crystal changed from 4.51 W / (m K) to 2.80W/ (m K). Secondly, Cr,Nd:GSAG crystals with diameter 桅 30mm were successfully grown by Czochralski method with 0.1 at% Cr3 in Nd:GSAG. The strongest absorption peak is located at 808.6nm, and the absorption cross section is 3.38 脳 10 ~ (-20) cm ~ (2). Regardless of the overlapping absorption bands of Nd3 and Cr3 in the Cr,Nd:GSAG absorption spectra, the intensity parameter 惟 t (ttn2m2m2h2) of Nd3 in Cr,Nd:GSAG is 0.380 脳 10-20cm2n ~ (2) 2.286 脳 10 ~ (-20) cm ~ (2) C ~ (2 +) 3.306 脳 10 ~ (-20) cm _ (2) C _ (2) C ~ (2 +) emission peak is located at 1060nm, and the emission cross section at 1060 nm is 5.98 脳 10 ~ (-20) cm ~ (-2) ~ (2) (2.60 脳 10 ~ (-20) cm ~ (-2) respectively. The 4F3/2 lifetime of Cr,Nd:GSAG at room temperature is 274 渭 s ~ (-1). The 808nm CW semiconductor laser (LD) is used as the pump source to study the 1.06 渭 m laser performance of the Cr,Nd:GSAG of 2mm 脳 2mm 脳 6mm. The threshold value is 1.233 W, the slope efficiency is 6.73 W, the maximum output power is 0.513 W, and the optical-optical conversion efficiency is 5.78 W. (3) Nd:GSAG and Cr,Nd:GSAG were irradiated by 60Co gamma ray source. The absorption of irradiated and unirradiated samples was compared with that of unirradiated samples. The results showed that the two crystals may have the ability to resist irradiation. Doping Cr3 is beneficial to enhance the radiation resistance of Nd:GSAG.
【學(xué)位授予單位】:中國科學(xué)技術(shù)大學(xué)
【學(xué)位級別】:碩士
【學(xué)位授予年份】:2017
【分類號】:O734
【參考文獻】
相關(guān)期刊論文 前10條
1 郭凱;駱軍;趙景泰;;熱電材料的基本原理、關(guān)鍵問題及研究進展[J];自然雜志;2015年03期
2 張鵬;王寧;于善偉;王奇;;兩種導(dǎo)熱系數(shù)檢測方法的差異[J];品牌與標準化;2012年06期
3 高進云;張慶禮;殷紹唐;劉文鵬;羅建喬;王迪;江海河;;大尺寸Nd~(3+):GGG激光晶體的單胞參數(shù)計算和組分分析[J];人工晶體學(xué)報;2011年02期
4 孫晶;李昌立;于文生;李四海;張大龍;劉景和;;化學(xué)腐蝕法研究Nd:YAG晶體位錯[J];人工晶體學(xué)報;2009年06期
5 曾繁明;張瑩;孫晶;劉景和;;摻釹釓鎵石榴石激光晶體光譜分析[J];光譜學(xué)與光譜分析;2009年05期
6 ;Segregation during crystal growth from melt and absorption cross section determination by optical absorption method[J];Science in China(Series G:Physics,Mechanics & Astronomy);2008年05期
7 張帥一;黃春霞;于果蕾;劉輝蘭;孫堯;李健;;激光二極管端面抽運激光晶體的熱效應(yīng)[J];中國激光;2008年03期
8 鄧建兵;張金濤;舒水明;段宇寧;;固體材料導(dǎo)熱率測量標準裝置的研究[J];現(xiàn)代測量與實驗室管理;2006年05期
9 廖毅;;空間輻照環(huán)境及紅外光子探測器的輻照效應(yīng)[J];紅外;2006年05期
10 孫敦陸,張慶禮,王愛華,杭寅,張連瀚,錢小波,祝世寧,殷紹唐;高濃度摻Er~(3+)鈮酸鋰晶體的光譜參數(shù)計算[J];光譜學(xué)與光譜分析;2005年09期
相關(guān)碩士學(xué)位論文 前10條
1 李慧;窄線寬1336.6nm激光技術(shù)研究[D];北京理工大學(xué);2015年
2 李寧;熱電氧化物鈦酸鍶的熱傳導(dǎo)研究[D];廈門大學(xué);2014年
3 周玉華;X射線Rietveld法測定納米鋁粉中單質(zhì)鋁含量及微觀應(yīng)力的研究[D];華中科技大學(xué);2012年
4 李現(xiàn)霞;基于近場輻射的介電薄膜熱導(dǎo)率模型研究[D];青島理工大學(xué);2010年
5 朱睿;天然方解石晶體電注入著色及光譜特性[D];天津大學(xué);2010年
6 范澤;摻釹硅酸鎵鑭(Nd:LGS)晶體生長及其性質(zhì)研究[D];山東大學(xué);2010年
7 滑文強;LD端面泵浦激光熱效應(yīng)研究[D];山東師范大學(xué);2010年
8 程蘇丹;銦摻雜β-Zn_4Sb_3晶體結(jié)構(gòu)的Rietveld精修[D];武漢理工大學(xué);2010年
9 孫峰;Rietveld方法精修及定量分析研究[D];中國海洋大學(xué);2009年
10 楊喜英;X射線衍射-Rietveld全譜圖擬合法測定粉塵中游離SiO_2含量的研究[D];廣西大學(xué);2008年
,本文編號:2275779
本文鏈接:http://sikaile.net/shoufeilunwen/benkebiyelunwen/2275779.html