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Nd:GdVO_4热常数的测量和激光性能研究 总被引:2,自引:0,他引:2
中频感应加热提拉法生长了低钕掺杂的GdVO_4晶体,用机械分析仪来测量Nd:GdVO_4晶体的热膨胀系数,沿c方向的热膨胀系数为7.42×10~(-6)/K,而沿α方向的热膨胀系数只有1.05×10~(-6)/K,比同比Nd_(0.0045)Y_(0.9946)VO_4晶体样品测量结果小。差示扫描热计法测量了Nd:GdVO_4晶体的比热,298K时为0.52J/g·K。首次用激光脉冲法测量了Nd:GdVO_4晶体的室温热导率。实验表明,Nd:GdVO_4晶体沿<001>方向的热导率数值达11.4W/m·K,比Nd:YAG晶体高(测得10.7W/m·K),其<100>方向的热导率为10.1W/m·K。激光实验显示在较高功率泵浦激光输出上Nd:GdVO_4晶体具有比Nd:YVO_4晶体更加优良的性能。 相似文献
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Nd∶GdVO4热常数的测量和激光性能研究 总被引:1,自引:0,他引:1
中频感应加热提拉法生长了低钕掺杂的GdVO4晶体,用机械分析仪来测量Nd∶GdVO4晶体的热膨胀系数, 沿c方向的热膨胀系数为7.42×10-6/K,而沿a方向的热膨胀系数只有1.05×10-6/K,比同比Nd0.0054Y0.9946VO4晶体样品测量结果小.差示扫描热计法测量了Nd∶GdVO4晶体的比热, 298K时为0.52J/g*K.首次用激光脉冲法测量了Nd∶GdVO4晶体的室温热导率.实验表明,Nd∶GdVO4晶体沿<001>方向的热导率数值达11.4W/m*K, 比Nd∶YAG晶体高(测得10.7W/m*K),其<100>方向的热导率为10.1W/m*K.激光实验显示在较高功率泵浦激光输出上Nd∶GdVO4晶体具有比Nd∶YVO4晶体更加优良的性能. 相似文献
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Nd:GdVO4激光晶体的光谱性质和热学性质 总被引:1,自引:2,他引:1
用提拉法生长了Nd:GdVO4单晶,测量了其室温吸收谱和室温荧光谱,测量了其热扩散系数α和比热Cp,从而得到了其热导率λ。可以看到Nd:GdVO4晶体的吸收波长在808nm附近,与已经商品化的GaAlAs LD的发射波长能很好地匹配,从而增加了吸收效率,并且Nd:GdVO4晶体具有较高的热导率,有望在高功率的激光系统中获得应用。所以Nd:GdVO4晶体是理想的激光材料。 相似文献
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Nd:GdVO4热常数的测量和激光性能研究 总被引:1,自引:1,他引:1
中频感应加热提拉法生长了低钕掺杂的GdVO4晶体,用机械分析仪来测量Nd∶GdVO4晶体的热膨胀系数, 沿c方向的热膨胀系数为7.42×10-6/K,而沿a方向的热膨胀系数只有1.05×10-6/K,比同比Nd0.0054Y0.9946VO4晶体样品测量结果小.差示扫描热计法测量了Nd∶GdVO4晶体的比热, 298K时为0.52J/g*K.首次用激光脉冲法测量了Nd∶GdVO4晶体的室温热导率.实验表明,Nd∶GdVO4晶体沿<001>方向的热导率数值达11.4W/m*K, 比Nd∶YAG晶体高(测得10.7W/m*K),其<100>方向的热导率为10.1W/m*K.激光实验显示在较高功率泵浦激光输出上Nd∶GdVO4晶体具有比Nd∶YVO4晶体更加优良的性能. 相似文献
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替代M-型钡铁氧体纳米粒子的微波吸收性能 总被引:12,自引:0,他引:12
The microwave-absorbing behavior of substituted M-type barium ferrite nano-particles was investigated. The nano-particles were synthesized with coprecipitation-melted salt method. For the purpose of comparison, corre-sponding micro-particles were also prepared through direct coprecipitation and sintering. XRD and TEM of the nano-particles showed that the ferrite was hexagonal in structure and widely distributed in size with particle size being less than 100nm, the complex permittivity and permeability of a 1.50mm thick specimen and a 1.40mm thick specimen containing 60% by weight of substituted M-type barium ferrite nano-particles and micro-particles were measured respectively in X band (8.2~12.4GHz) range, from which the reflection loss (R.L.) of microwaves was calculated and two comparative absorption curves were given. The results showed that the synthetic nano-particles could well absorb microwaves in X band. The absorption was larger than 10dB in the range of 9.2~12.4GHz while the maximum absorption was 38.6dB at 10.6GHz. 相似文献
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Czoehralski法成功生长了一系列不同Cd/Y的低掺杂Nd:YxGd1-xVO4混晶,并对它们的一些基本性质进行了比较,发现随着Gd含量的增加,晶体晶胞a,c轴常数呈线性增长,故YVO4和GdVO4晶体可以实现无限互溶。少量Gd掺杂可使混晶晶体比热和荧光寿命增大,并有效地增强了其荧光强度。我们对该晶体的低功率泵浦下的Cr^4 :YAG调Q激光性能也进行了研究,发现Nd:YxGd1-xVO4混晶具有良好调Q性能。 相似文献
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Nd0.007Gd0.993VO4晶体折射率和折射率温度系数的测量 总被引:3,自引:1,他引:3
利用自准直法,在20℃到170℃温度范围和0.4880μm、0.6328μm、1.0640μm、1.0795μm、1.3414μm等波长测量了Nd0.007Gd0.993VO4晶体的折射率,得到了这种晶体的Sellmeier方程和折射率温度系数.为了验证得到结果的可靠性,利用得到的Sellmeier方程计算1.0640μm的寻常光和异常光的折射率,并与实验测量的结果进行比较,两者的差异不大于2.2×10-4,处在测量误差的范围内.测量结果表明在室温下,对1.0640μm波长的双折射率为0.2201,双折射率温度变化率为4.3×10-6/℃.因此,与YVO4相仿,这种晶体不仅是一种优秀的激光基质材料,而且是一种优秀的双折射晶体. 相似文献
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Diode-pumped Nd:YxGd1-xVO4 crystal continuous-wave laser 总被引:3,自引:0,他引:3
The diode-pumped Nd:YxGd1-xVO4 crystal continuous wave (CW) laser operating at 1.06 μm with a simple plane-concave cavity and a "V-shaped" folded cavity for intracavity frequency-doubling have been studied. With the incident pump power of 8 W, an output power (1.06 μm) of 3.4 W was achieved,giving an optical conversion efficiency of 42.5%. 884 mW of stable green radiation was generated with the incident pump power of 5.9 W, giving an optical conversion efficiency of 15%. 相似文献