253 resultados para Cr : Yb : YAG crystal

em Chinese Academy of Sciences Institutional Repositories Grid Portal


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The fluorescence emission spectra of Cr:Yb:YAG crystal are measured and the effective stimulated emission cross section of the crystal are obtained from -80 degrees C to +80 degrees C. A linear temperature dependence between -80 degrees C and +80 degrees C is reported for the 1.03 mu m peak stimulated emission cross section of Cr:Yb:YAG crystal. (c) 2004 Elsevier B.V. All rights reserved.

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用光纤耦合激光二极管抽运Cr,Yb:YAG晶体获得了1.03 μm的自调Q激光输出,输出的调Q脉冲非常稳定,抽运阈值功率为680 mW,脉冲宽度为3.3 ns,获得的平均功率为156 mW,斜率效率为18.5%。随着抽运功率的增大,重复频率成线性增长,而脉宽略有减少,单脉冲能量和峰值功率都始终呈增大趋势。光束质量因子M2为1.17。

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The fluorescence emission spectra of Cr:Nd:YAG crystal are measured and the effective stimulated emission cross-section of the crystal is obtained from -80 to +80 degrees C. A linear temperature dependence between -80 and +80 degrees C is reported for the 1.064-mu m peak stimulated emission cross-section of Cr:Nd:YAG crystal. (C) 2005 Elsevier Ltd. All rights reserved.

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研究了室温下YbYAG的上转换荧光光谱,此荧光归因于Yb^3+离子的“合作”发光和Yb抖离子到稀土杂质离子的能量转移。测试了YbYAG晶体的X射线荧光,发光峰对应于电荷迁移态到Yb^3+离子的基态、激光态间的跃迁。研究了CrYbYAG晶体的荧光光谱。讨论了Cr^4+激光输出的可能性。

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The Cr(0.1%),Yb(10%):GGG crystals have been grown by the Czochralski method. The chemical composition is: Yb0.33Gd2.47Cr0.005Ga5.2O12. There are no observed Yb3+ ions substituting Ga3+ ions, just like that of Yb:GGG crystals. The defects in Cr,Yb:GGG crystal were also investigated. The absorption and emission spectra of Cr,Yb:GGG crystal at room temperature have been measured. The 02 and H-2 annealing effect of Cr,Yb:GGG crystal have been compared. Cr3+ can greatly weak the visible luminescence of this crystal. The Cr-Yb-codoped crystals may be potential materials for compact, efficient, high stability LD pumped solid state lasers. (C) 2006 Elsevier B.V. All rights reserved.

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By using a continuous-wave Ti:sapphire laser as a pumping source, we demonstrated a passively Q-switched Yb:YAG laser at room temperature with Cr4+:YAG as the saturable absorber. We achieved an average output power of as much as 55 mW at 1.03 mum with a pulse width (FWHM) as short as 350 ns. The initial transmission of the Cr4+:YAG has an effect on the pulse duration (FWHM) and the repetition rate of the Yb:YAG passively Q-switched laser. The Yb:YAG crystal can be a most promising passively Q-switched laser crystal for compact, efficient, solid-state lasers. (C) 2001 Optical Society of America.

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用脉冲电子束激发测量了不同Yb^3+掺杂浓度的YbYAG晶体的红外(IR)闪烁发光性能。YbYAG晶体的IR闪烁发光具有高的光产额和长的衰减时间,但存在浓度猝灭效应和温度依赖关系。YbYAG晶体的IR闪烁性能还与晶体品质有关,相同掺杂浓度的YbYAG晶体,品质优异的会获得更高的光产额。这一初步的研究成果表明,部分掺Yb^3+晶体有可能用于医学成像装置。

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通过不同Yb^3+掺杂浓度(5%-30%,原子数分数)的YbYAG晶体的阴极射线发光谱、衰减时间、光输出及其温度依赖关系的测量,研究了YbYAG晶体的闪烁性能。不同Yh^3+掺杂浓度的YbYAG晶体具有不同的光输出和猝灭温度,光输出随Yb^3+掺杂浓度的增大而降低,猝灭温度则随掺杂浓度的增大而升高。室温下YbYAG晶体的发光衰减时间较短,均小于50ns。Yb^3+掺杂浓度为5%的YbYAG晶体具有较高的光输出和较低的猝灭温度。

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The 10at% Yb-YAP crystal has been grown by the Czochralski method. The absorption and emission spectra and fluorescence lifetime of Yb:YAP crystal at room temperature were studied. There is a strong absorption band centered at 959 nm and the absorption cross-section of 1.51 × 10-20 cm2. The emission cross-section at 1040 nm is 0.6 × 10-20 cm2 and the fluorescence lifetime is about 1.2 ms. The effects of O2-annealing on the spectral properties were studied. The spectroscopic properties strongly depended on the axis direction and b axis was the best direction for laser output. The spectrum parameters of Yb:YAP and Yb:YAG crystal were compared.}

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应用中频感应提拉法生长出掺杂浓度为10 at.-%的Yb:YAGYb:YAP晶体,对比了室温下两种晶体的吸收和发射光谱特性。结果表明,Yb:YAG晶体比Yb:YAP晶体有更好的激光性能和低的阈值;同时对比发现,Yb:YAP晶体的吸收截面是Yb:YAG晶体的2.16倍,它容易实现LD泵;由于Yb:YAP晶体的各向异性,它有轴向效应明显,它可以产生偏振激光。

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The YAG crystal codoped with Yb3+ and Tm3+ has been grown by Czochralski (Cz) method. The crystal structure of the crystal has been determined by X-ray diffraction analysis. The absorption and emission spectra of Yb,Tm:YAG crystal at room temperature have also been studied. The emission cross-sections have been calculated by Fuechtbauer-Ladenburg formula and reciprocity method. (C) 2007 Elsevier B.V. All rights reserved.

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介绍了近几年迅速发展的一种新型激光介质——透明Nd:YAG多晶陶瓷的发展状况,对比分析了多晶陶瓷与单晶的光谱特性、激光特性和连续实验研究情况。并对钛宝石激光器调谐至808nm,端面抽运Nd:YAG陶瓷被动调Q全固态激光器的脉冲运转进行了较为详细的理论分析和实验研究。采用初始透射率为90%的Cr^4+:YAG可饱和吸收晶体,被动调Q的阈值功率为119mW,当端面抽运功率为465mW时,获得波长为1064nm,脉宽为16ns,重复频率为18.18kHz,单脉冲能量为3.4μJ,平均输出功率为61mW的稳定调Q

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报道了激光二极管(LD)抽运的Nd:YLF激光器,采用平凹腔结构,分别用两片Cr^4+:YAG可饱和吸收晶体,实现了被动调Q,输出激光波长为1053nm。采用厚度为0.5mm小信号透过率为90%的Cr^4+ YAG,在泵浦功率最大为17W时,输出脉冲宽度为60.6ns,平均功率为1.5W,重复频率为9.5kHz,单脉冲能量为157.9mJ;采用厚度为0.55mm小信号透过率为95%的Cr^4+ YAG,在泵浦功率最大为17W时,输出脉冲宽度为68.6ns,平均功率为1.35W,重复频率为14kHz,单脉冲

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We report what is believed to be the first demonstration of the laser action of Yb3+ -doped Gd2SiO5 (Yb:GSO) crystal pumped by a 940-nm laser diode at room temperature. The threshold of laser generation is only 0.85 kW/cm(2), which is smaller than the theoretic threshold of Yb:YAG (1.54 kW/cm(2)). The laser wavelength is 1090 mn. With a 2.5% output coupler, the maximum output power is 415 mW under a pump power of 5 W. By using the SESAM, the Q-switched mode locking and CW mode-locked operations are demonstrated.

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The Yb (10%):GGG and Yb (30%): GGG crystals have been grown by the Czochralski method. The chemical compositions are: Yb1.07Gd1.74Ga5.19O12 and Yb0.33Gd1.47Ga5.2O12. The absorption and emission spectra of Yb:GGG crystal at room temperature have been measured. The spectroscopic parameters of Yb:GGG and Yb:YAG have been compared. Optical absorption spectra of Yb:GGG show 4f-4f transitions related to Gd3+ ion around 300 nm, and also an onset of charge transfer (CT) transitions from oxygen ligands to Gd3+ or Yb3+ cations below 240nm. The CT absorption of Yb3+ is largely overlapped by that of Gd3+ ions. (c) 2005 Elsevier B.V. All rights reserved.