Highly efficient,tunable, ultrabroadband NIR photoemission from Bi-doped nitridated germanate glasses toward all-band amplification in optical communication

Bismuth(Bi)-doped near-infared(NIR) glass that can cover the entire optical communication window(850, 1310, and1550 nm) has become the subject of extensive research for developing photonic devices, particularly, tunable fiber lasers and ultrabroadband optical amplifiers. However, the realization of highly efficient NIR luminescence from Bi-doped glass is still full of challenges. Notably, due to the co-existence of multiple Bi NIR centers in the glass, the origin of newly generated Bi NIR emissi...     

三层材料纳米颗粒形状对消光特性的影响

通过高分辨率电子束光刻方法制备了不同形状的三层复合材料纳米颗粒,研究了这种纳米颗粒的形状变化对消光特性的影响。测试结果表明,当入射波偏振方向平行于短轴时,随着长宽比的增大,共振峰位置发生蓝移;当光源偏振方向平行于长轴时,随着长宽比的增大,共振峰位置发生红移。还用时域有限差分算法以及表面等离波子的Lorentz模型对纳米颗粒的消光特性进行数值计算,所得的消光频谱曲线、共振峰位置变化趋势与实验基本一致。此外,还研究了主体材料层厚度对消光特性的影响,发现其厚度在20～90nm变化时,共振峰发生3～115nm的蓝移。     

飞秒激光相干场诱导材料功能微结构

飞秒激光在整个脉冲宽度内具有极好的相干性，因而当从同一光束分出的两束或两束以上的光束时间与空间上实现相互叠加时将会形成强度周期性调制的电磁场．这种周期调制的电磁场与材料产生相互作用，能诱导出相应的周期微结构．最近通过两束或两束以上飞秒激光干涉诱导功能微结构得到了广泛研究．文章综合了国内外飞秒激光研究小组在干涉诱导微结构方面的一些最新成果以及作者在这方面开展的工作，对飞秒激光干涉技术的原理及其在诱导微结构方面的应用进行了介绍．     

掺铒高硅氧玻璃光谱性质的研究

应用Judd-Oflet理论计算了新型掺铒高硅氧玻璃中铒离子的强度参量Ω_t(t=2,4,6)，Ω₂=8.15×10^-20，Ω₄=1.43×10^-20，Ω₆=1.22×10^-20，相比于其他氧化物玻璃，表现出较大的Ω_2,6值，反映了铒离子周围的近邻结构不对称性和Er-O键的离子键成分较高.利用McCumber理论计算得到了能级^{关键词： 掺铒高硅氧玻璃 Judd-Ofelt理论 量子效率}     

Self-formation of void femtosecond array in Al2O3 crystal by laser irradiation

The femtosecond laser induced void array inside Al2O3 crystals was discussed. The void array was formed spontaneously under the irradiation of a single beam of infrared femtosecond laser which was focused at a fixed point inside the Al2O3 crystal sample. It was found that the regular voids only could be fabricated near the sample surface, which was different from the situation in CaF2 single crystal reported before. The possible mechanism of the phenomena was also discussed.     

高浓度CO2气氛下燃煤氮、硫污染物的释放特性

采用污染物在线分析仪、气相便携红外分析仪研究了程序升温条件下改变氧化介质时煤中氮,硫的释放特性以及含硫物相的浓度变化规律,探讨了不同气氛,CO2浓度与O2浓度单独变化时对NO、SO2析出特性的影响机理.结果表明:O2/CO2燃烧气氛下NO、SO2排放峰值及总量均低于O2/N2气氛.CO2气氛下烟气中存在大量的CO,有利于NO的降解,同时也促进了烟气中其他含硫物相的形成,随着CO2浓度的增加,特别是在燃烧后期,NO、SO2的排放显著降低.O2浓度改变对NO和SO2的释放影响不同:O2浓度升高促进了SO2的析出;但是O2浓度在一定范围内增加对NO的排放并无明显影响,随着O2浓度进一步增加,NO的释放峰向低温区迁移,同时排放量降低.     

Broadband Infrared Luminescence from Bismuth-Doped GeS2--Ga2S3 Chalcogenide Glasses

Near-infrared luminescence is observed from bismuth-doped GeS2-Ga2Sa chalcogenide glasses excited by an 808 nm laser diode. The emission peak with a maximum at about 1260 nm is observed in 80GeS2-2OGa2 Sa：O.fBi glass and it shifts toward the long wavelength with the addition of Bi gradually. The full width of half maximum （FWHM） is about 200 nm. The broadband infrared luminescence of Bi-doped GeS2-Ga2Sa chalcogenide glasses may be predominantly originated from the low valence state of Bi, such as Bi＋. Raman scattering is also conducted to claxify the structure of glasses. These Bi-doped GeS2 Ga2Sa chalcogenide glasses can be applied potentially in novel broadband optical fibre amplifiers and broadly tunable laser in optical communication system.     

用飞秒激光在α-BBO晶体中诱导析出β-BBO相

通常超快强激光主要用于研究发生在材料内部,时间尺度在皮秒(10^-2s)到飞秒(10^-15s)范围内的动力学现象。然而,其极短的脉冲宽度,使得激光束经聚焦后在焦斑处的功率强度可达10^14W／cm^2。所以,当这种激光束被聚焦在透明材料的内部时,巨大的能量可在极短的时间内积聚在非常小的区域内,并使该区域内的温度和内压力急剧上升。     

Femtosecond Laser-Written Waveguides in a Bismuth Germanate Single Crystal

We demonstrate the fabrication of symmetric waveguides in a bismuth germanate （BGO） single crystal using a double line approach by an 80Ohm [emtosecond laser. The optical attenuation of the single mode waveguide is measured to be 4.2 dB/cm at 633nm. The influence of pulse energy and focal depth on the end facet of the irradiated region is also studied. This technique is promising to fabricate buried BGO waveguide arrays used in positron emission tomography systems.     

再燃降低NO_x排放及煤粉燃尽特性研究

以包含两种低挥发份贫煤在内的四种煤作为主燃料,在一维炉和一台93 kW卧式单角炉上对气体燃料再燃过程及煤粉和再燃燃料的燃尽特性进行了详细实验研究,同时对炉膛内NO_x浓度分布等进行了测量和分析.实验发现,再燃过程除了要采用合适再燃区停留时间外,气体再燃燃料还应选择在炉膛内NO_x浓度较大区域内喷入,以提高再燃脱硝效率.实验结果表明,即使采用低挥发份煤作为主燃料,当再燃区停留时间达到约0.7～0.9 s,气体再燃燃料比例达到10%～15%时,气体燃料再燃过程就能在保证煤粉颗粒燃尽率不明显降低前提下,获得50%以上的再燃脱硝效率.