LD泵浦Nd:YVO_4/KTP激光器晶体长度对输出的影响

利用四能级激光系统的速率方程 ,对激光二极管 (LD)纵向泵浦Nd :YVO4 /KTP腔内倍频绿光激光器激活介质和倍频晶体的长度对输出激光功率的影响进行了理论计算 ,给出了参数优化结果 ,分析了它的工作特性 ,得到与理论计算符合较好的实验结果。     

自启动、低功率泵浦的自锁模Ti：蓝宝石激光器和它的高效连续运转

报道了一台自启动、长时间稳定、低功率泵浦的自锁模Ｔｉ：蓝宝石激光器和它的高效连续运转的实验结果．实验中观测到５３ｎｍ的光谱带宽（ＦＷＨＭ）．此谱宽可支持１３ｆｓ的激光脉冲．受自相光仪测量仪器的限制．测得的脉宽为２４．６ｆｓ．实际脉冲脉宽可能小于２０ｆｓ．此激光器在自启动锁模、低功率泵浦时．脉宽小于５０ｆｓ．激光器在连续运行时获得０．２Ｗ的泵浦阈值．３５％的斜率效率和１．１Ｗ的激光输出（４Ｗ泵浦）．     

H optimal approximation for causal spline interpolation

In this paper, we give a causal solution to the problem of spline interpolation using H^∞ optimal approximation. Generally speaking, spline interpolation requires filtering the whole sampled data, the past and the future, to reconstruct the inter-sample values. This leads to non-causality of the filter, and this becomes a critical issue for real-time applications.Our objective here is to derive a causal system which approximates spline interpolation by H^∞ optimization for the filter. The advantage of H^∞ optimization is that it can address uncertainty in the input signals to be interpolated in design, and hence the optimized system has robustness property against signal uncertainty.We give a closed-form solution to the H^∞ optimization in the case of the cubic splines. For higher-order splines, the optimal filter can be effectively solved by a numerical computation. We also show that the optimal FIR (finite impulse response) filter can be designed by an LMI (linear matrix inequality), which can also be effectively solved numerically. A design example is presented to illustrate the result.     

Eu^2＋在KCaPO4中的发光及晶体学格位

采用高温固相法制备了KCaPO4：Eu^2＋蓝绿色荧光粉,研究了材料的发光特性。在400 nm近紫外光激发下,材料呈非对称的单峰发射,主峰位于487 nm。监测487 nm发射峰,对应的激发光谱覆盖300-450 nm,说明材料能够很好的吸收紫外-近紫外光,发射蓝绿色光。利用van Uitert公式计算了Eu^2＋取代...     

溶胶-凝胶法制备Al3+掺杂ZnO薄膜的结构和光学性能

采用无机盐溶胶-凝胶方法在载玻片衬底上制备了ZnO:Al薄膜,利用X射线衍射(XRD)、紫外-可见光透射光谱(UV-Vis transmittance spectrum)和扫描电镜(SEM)研究了退火温度和Al3+掺杂浓度对ZnO:Al薄膜结构和光学性能的影响.结果表明,随退火温度的升高或进行适当浓度的Al3+掺杂,可...     

Gate‐Controlled Energy Barrier at a Graphene/Molecular Semiconductor Junction

The formation of an energy‐barrier at a metal/molecular semiconductor junction is a universal phenomenon which limits the performance of many molecular semiconductor‐based electronic devices, from field‐effect transistors to light‐emitting diodes. In general, a specific metal/molecular semiconductor combination of materials leads to a fixed energy‐barrier. However, in this work, a graphene/C₆₀ vertical field‐effect transistor is presented in which control of the interfacial energy‐barrier is demonstrated, such that the junction switches from a highly rectifying diode at negative gate voltages to a highly conductive nonrectifying behavior at positive gate voltages and at room temperature. From the experimental data, an energy‐barrier modulation of up to 660 meV, a transconductance of up to five orders of magnitude, and a gate‐modulated photocurrent are extracted. The ability to tune the graphene/molecular semiconductor energy‐barrier provides a promising route toward novel, high performance molecular devices.     

热效应不敏感的Nd:GdV04/KTP全固态绿光激光器设计

利用基于传播圆变换理论的图解分析方法,得到了具有激光晶体热透镜不敏性的V形折叠腔参数.实验中通过LD端面泵浦Nd:GdVO4,获得了稳定的TEM<,∞>模激光输出.将非线性晶体KTP置于基波的腰斑处,在19.7W的注入泵浦功率下获得了3.68W的531.5nm连续绿光激光输出,考虑到泵浦耦合用准直聚焦筒10%的耦合损耗,实现光一光转换率21%.经测量该激光腔输出功率及热稳定性在国内LD泵浦全固态连续绿光激光器研究领域处于领先水平.     

掺钛蓝宝石晶体激光放大实验研究

报道了掺钛蓝宝石晶体激光放大实验研究，实验中得到最大的单程放大和双程放大增益分别为１４．７６和２６．３１，对应双程放大的增益系数为１．８１ｃｍ－１，并由此推算出掺钛蓝宝石晶体的增益截面为２．７４×１０－１９ｃｍ２，饱和能量密度为０．９３Ｊ／ｃｍ２．并给出不同的泵浦能量密度所对应的最佳放大介质长度。实验表明小信号近似下，放大增益只与泵浦功率密度有关．与注入种子能量无关。实验还测量了掺钛蓝宝石晶体对不同波长种子光的放大增益。     

高峰值功率自准直脉冲Nd:YAG激光加工无锥度直孔研究

利用改进的脉冲Nd:YAG激光器,对激光冲击打孔加工无锥度直孔进行了实验研究。在优化激光脉冲峰值功率和脉冲能量、辅助气压参数的基础上,通过比较实验证明,能量递增组合脉冲是实现无锥度直孔加工的有效方式,增加脉冲组合中脉冲的个数可加工出负锥度的孔;激光焦点位置是影响孔锥度的重要因素,焦点位于材料表面上方1.1~1.7 mm有利于减小锥度。在厚度为1.5,3.0 mm的镍基高温合金材料上,获得孔径分别为480,510μm的直孔,重复打孔孔径误差约30μm,孔锥度<1%。给出了可实用于激光冲击打孔的直孔加工方法和脉冲激光器,并可用于其他材料的加工。     

YAG激光器泵浦钛宝石激光器和光学参量振荡器

采用一台调Q脉冲式Nd：YAG激光器同时泵浦Ti：蓝宝石激光器和光学参量振荡器（OPO），在重复频率30Hz下获得了Ti：蓝宝石可调谐激光波长为700～890nm，转换效率28．8％及440～2600nm的连续可调谐窄线宽的光参量激光输出，能量转换效率达23％。