欢迎登录材料期刊网

材料期刊网

高级检索

由于Nd3+离子半径0.112nm和Y3+离子半径0.101nm相差10.9%,使得Nd3+离子非常难于进入YAG晶体中.我们用温度梯度法生长了大尺寸高浓度(2.8at%)的Nd:YAG晶体,同时与用提拉法Nd:GGG晶体进行了比较.分析了高浓度掺杂Nd:GGG和 Nd:YAG晶体浓度猝灭问题.研究了不同浓度掺杂的猝灭效应.在同样的掺杂浓度下,我们发现它们的猝灭程度不同,其原因是两种晶体中ΔE(-)mism和ΔE(+)mism不同.

The ionic radius of Y3+ is 0.101nm and of Nd3+ is 0.112nm, a difference of about 10.9%. Therefore it is difficult to grow highly doped Nd:YAG. In this paper we have grown Large sized highly doped(2.8at.%) Nd:YAG crystals by TGT method. Large sized(φ>70mm) high quality Nd:GGG crystals have been grown by CZ method for comparison at the same time. The concentration quenching in Nd:GGG crystals with high Nd3+ doping level was demonstrated and studied as well. The comparisons of the concentration quenching effects between the Nd:GGG and Nd:YAG crystals have been listed. The reason why GGG crystal has weaker concentration quenching effect than YAG crystals may be that: YAG crystal has a stronger field strength than that of GGG crystal, which leads to higher values of ΔE(-)mism and ΔE(+)mism in GGG crystal and this causes weaker concentration quenching effect in Nd:GGG crystal.

参考文献

[1] John Vetrovec.Gain Media for High-average Power Solid-state lasers[A].Poland
[2] John Vetrovec.Solid-state Scalable to Ultrahigh-average Power[A].Poland
[3] John Vetrovec.Materials for High-average Power Solid-State Laser[M].SPIE LASE,2003:26-31.
[4] Giesen G;Hugel H;Voss A et al.Scalable Concept for Diode-pumped High Power Solid-state Lasers[J].Applied Physics B-Lasers and Optics,1994,58:365-372.
[5] Stewen C;Contag K;Larionov M et al.A 1-kW CW Thin Disk Laser[J].IEEE Journal of Selected Topics in Quantum Electronics,2002,6:650-657.
[6] 张连翰,杭寅,孙敦陆,钱小波,李世锋,殷绍唐.Nd3+∶Y0.5Gd0.5VO4晶体光谱特性[J].中国激光,2004(03):339-341.
[7] Alexander A.Kaminskii.Laser Crystal[M].NewYork.Springer-verlag Berlin Heidelberg,1981
[8] Albrecht G;George E V;William F K et al.High Energy Bursts from Solid State Laser Operated in the Heat Capacity Limited Regime[P].US 5526372
[9] Hoffmann H J;Glaswerke S .Solid State Laser Rods for High Power Conditions[P].US 4845721
[10] Cao Weilou;Zhang Meizhen;Hua Xuelei .Output Characteristics of Large Aperture Nd:YAG Disk Laser[J].Acta Optica Sinica,1988,8(08):711-716.
[11] Eunchong Kanchanavaleerat;Didier Cochet-Muchy;Milan Kokta;Jennifer Stone-Sundberg;Paul Sarkies;Julian Sarkies;Jonathan Sarkies .Crystal growth of high doped Nd:YAG[J].Optical materials,2004(4):337-341.
[12] Deng Peizhen;Qiao Jingwen;Hu Bing et al.Perfection and Laser Performances of Nd:YAG Crystals Grown by TGT[J].Journal of Crystal Growth,1988,92:276-286.
[13] Dong J;Deng P;Gan F et al.High Doped Nd:YAG Crystal Used for Microchip laser[J].Optics Communications,2001,197:413-418.
[14] Kazuo Maeda;Naoki Wada;Masami Umino et al.Concentration Dependence of Fluorescence Lifetime of Nd doped Gd3Ga5O12 lasers[J].Japanese Journal of Applied Physics,1984,23(10):759-760.
[15] Alexander A Kaminskii.Laser Crystal[M].New York:Springer-verlag Berlin Heidelberg,1981
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%