聚合物串联耦合双环电光开关的优化

利用耦合模理论、电光调制理论和微环谐振理论,提出一个聚合物串联耦合双环电光开关器件模型,在1.55 μm谐振波长下对该器件进行了模拟和优化.结果为：微环波导芯截面尺寸为1.6×1.6 μm2,波导芯与电极间的限制层厚度为1.6 μm,电极厚度为0.15 μm,微环半径为15.2 μm,微环与信道间的耦合间距为0.14 μm,微环与微环间的耦合间距为0.6 μm,输出光谱的3 dB带宽约为0.06 nm,开关电压约为6 V左右,插入损耗约为2.2 dB,串扰约为－20 dB.所设计的双环电光开关较单环型电光开关不仅输出光谱更加平坦陡峭,非谐振光更弱,而且开关电压更低.     

温度和质量浓度对硫酸气溶胶光学特性的影响

根据新版大气分子光谱资料集(HITRAN2008)中硫酸气溶胶的复折射指数资料,利用经典的Mie理论编写程序,计算不同温度和质量浓度下硫酸气溶胶粒子在10 μm和0.87 μm 2个波段的散射效率和散射相函数.结果表明,在10 μm波段,在相同的H_2SO_4/H_2O质量浓度下,温度越高,硫酸气溶胶的后向散射强度越强,即冷却作用越强;在相同的温度下,硫酸粒子的质量浓度越小,其后向散射越弱,冷却作用越弱.在0.87 μm波段,硫酸粒子质量浓度一定时,温度变化对硫酸粒子散射强度的影响不大;若温度一定,在散射角大于173°的后向方向,硫酸质量浓度越大,散射强度越小,其冷却效应越弱.     

1.30μm／1.55μm SiGe多模干涉滤波器

用多模干涉原理分析和设计了光通信波长（１．３０μｍ～１．５５μｍ）的Ｓｉ１－ｘＧｅｘ／Ｓｉ滤波器，并用模的传播分析方法对其传输特性进行了研究。结果发现，在Ｇｅ含量ｘ＝０．０４时，干涉区的脊高和宽度分别为６．３５μｍ和８μｍ。如果多模干涉区长度ＬＭ＝２３０２．５μｍ，可滤１．３０μｍ而通１．５５μｍ的波长。且具有３１ｄＢ的对比度和０．０１ｄＢ的插入损耗；如果多模干涉区长度ＬＭ＝２５１２．５μｍ，可滤１．５５μｍ而通１．３０μｍ的波长。具有１６ｄＢ的对比度和０．０９ｄＢ的插入损耗。     

Fabrications and characterizations of high performance 1.2 kV,3.3 kV,and 5.0 kV class 4H–SiC power SBDs

In this paper, 1.2 kV, 3.3 kV, and 5.0 kV class 4H–SiC power Schottky barrier diodes(SBDs)are fabricated with three N-type drift layer thickness values of 10 μm, 30 μm, and 50 μm, respectively. The avalanche breakdown capabilities,static and transient characteristics of the fabricated devices are measured in detail and compared with the theoretical predictions. It is found that the experimental results match well with the theoretical calculation results and are very close to the 4H–SiC theoretical limit line. The best achieved breakdown voltages(BVs) of the diodes on the 10 μm, 30 μm, and 50 μm epilayers are 1400 V, 3320 V, and 5200 V, respectively. Differential specific-on resistances(R_(on-sp)) are 2.1 m?·cm~2,7.34m?·cm~2, and 30.3 m?·cm~2, respectively.     

Spectral thermal emission of LiF slabs in the far infrared

The spectral thermal emission of LiF slabs on metallic substrate is measured for different polarizations in the wavelength region between 30 μm and 130 μm at a temperature of 523 K. The thickness of the slabs varies from 0.26 μm to 26 μm. We observe various resonances, whose number and positions depend on the thickness and the angle of the emitted radiation. The experimental results are compared with the theory of Kliewer and Fuchs.     

三维时域散斑动态干涉测量系统的集成化设计

三维电子散斑干涉技术（3D ESPI）具有非接触、高精度、高灵敏度和全场测量等优点,被广泛应用于许多领域。为了实现非接触动态全场三维测量,设计并建立了一个紧凑、完备的三维测量系统。用一个多波长光纤耦合激光器代替3个独立光源,产生的离面、面内散斑干涉图仅用一台彩色CCD相机就能捕捉和处理;整个测量系统采用笼式结构,具有高度的灵活性和稳定性;对基于小波变换的相位展开算法进行了编程,实现了被测物体三维位移信息的完整提取。实验证明该测量系统可以实时获取被测物体的三维位移,在测量实验中,获得的三维位移值17.68 μm、36.23 μm、13.85 μm,相比于实际位移值18.1 μm、36.4 μm、14.0 μm它们的绝对误差分别为0.42 μm、0.17 μm、0.15 μm,相对误差分别为2.3%、0.5%、1.1%。     

Coupled high Q-factor surface nanoscale axial photonics (SNAP) microresonators

We experimentally demonstrate series of identical two, three, and five coupled high Q-factor surface nanoscale axial photonics (SNAP) microresonators formed by periodic nanoscale variation of the optical fiber radius. These microresonators are fabricated with a 100 μm period along an 18 μm radius optical fiber. The axial FWHM of these microresonators is 80 μm and their Q-factor exceeds 10(7). In addition, we demonstrate a SNAP microresonator with the axial FWHM as small as 30 μm and the axial FWHM of the fundamental mode as small as 10 μm. These results may potentially enable the dense integration of record low loss coupled photonic microdevices on the optical fiber platform.     

基于差频技术产生4μm波长光波混频系统的特性分析

介绍了一种基于差频技术产生4μm中红外激光输出的技术方案。将Nd：YAG激光器产生的1．06μm和1．44μm的激光直接注入LiNbO3晶体中进行差频，从而得到4μm的激光输出。导出了处理三波耦合的耦合波方程，并作了计算分析。结果表明，该方案在4．04μm波长处的激光输出可达40-50mJ。     

Brillouin gain spectrum characterization in Ge-doped large-mode-area fibers

The dependence of Brillouin gain spectrum (BGS) characteristics, including the Brillouin frequency shift (BFS) and the BGS bandwidth, on germanium concentration in large-mode-area Ge-doped passive fibers is investigated theoretically and experimentally. The simulation results show that the BFS is inversely proportional to GeO₂ concentration, and the BGS bandwidth initially increases with the augment of GeO₂ concentration, and then decreases. The BGSs of four fibers with core diameters of 10 μm and 20 μm for different GeO₂ concentrations are compared experimentally. Experimental results demonstrate that with the same core diameter, the variations of BFS and BGS bandwidths with GeO₂ concentration accord with the simulation results. Additionally, the BGS characteristics of three large-mode-area passive fibers with diameters of 10 μm, 25 μm, and 30 μm are measured, which confirm that the increasing of the fiber diameters will cause the BGS bandwidth to broaden. We believe that these results can provide valuable references for modulating the high-power narrow-linewidth fiber lasers and Brillouin fiber amplifiers.     

冲击波作用下微米尺度金属颗粒群的动力学行为

基于平面化爆驱动飞片高压加载技术和激光测速技术,研究了冲击波加载不同粒径锡颗粒群的微喷射行为以及在空气中的减速规律.实验结果表明,锡颗粒的最快喷射速度随粒径增大而显著增大.通过对微喷射形成过程的三维光滑粒子流体动力学方法数值模拟发现,大粒径锡颗粒之间存在较大的空隙结构,冲击波与空隙结构的相互作用诱导产生高速汇聚射流,空隙结构越大对应的喷射速度也越高.此外,通过研究不同粒径颗粒在复杂流场中的减速规律,进一步深化了对微喷射破碎后的颗粒尺度状态以及混合输运特性的认识.研究结果对于预测和分析冲击波加载微米颗粒群的微喷混合特性具有一定价值.     

亚微米光栅型导光板设计

提出了利用亚微米光栅制作导光板的方法,给出亚微米光栅型导光板的初始结构.用严格耦合波理论计算分析了在满足基底全反射条件的45°入射角下红(700 nm)、绿(555 nm)、蓝(465 nm)三色光垂直出射的亚微米光栅(0.651μm、0.516μm、0.433μm)在槽深0.05~0.9μm之间变化时,透射衍射效率在2%~43%之间变化.分析了亚微米光栅的作用,做出性能评价,并研究了特定范围入射角引起的衍射角变化.     

Low-loss chalcogenide waveguides on lithium niobate for the mid-infrared

We demonstrate low-loss chalcogenide (As(2)S(3)) waveguides on a LiNbO(3) substrate for the mid-IR wavelength (4.8 μm). Designed for single-mode propagation, they are fabricated through photolithography and dry-etching technology and characterized on a mid-IR measurement setup with a quantum cascade laser. For straight waveguides, propagation loss as low as 0.33 dB/cm is measured and low-loss bends on the order of 100 μm are simulated, with measurement results showing <3 dB for a 250 μm bend radius. The coupling efficiency is estimated to be 81%. In addition, the influences of variations in width and bend radius are also investigated.     

Optimization of SPRITE detectors

The optimized operating parameters of SPRITE detector working band in the 8–14 μm region have been calculated by computer modeling based on one dimensional theory. The results suggest the length of filaments should be 700 μm; the width 50 μm; the thickness 7 μm; the length of read-out area 50 μm and the bias voltage 2.8 V. The optimized outline curve of the read-out area has also been obtained by use of a variational method: Y = 7.5 cosh (0.04211X). This results in a significant reduction of transit time and transit time dispersion from 0.26 to 0.20 μs and 0.13 to 0.045 μs, respectively.     

Study on the Range of Particles Size Measured by Backscattering Method in Visual‐infrared Incident Spectrum

For the measurement of particles size with backscattering method, the suitable range of particles size measurement have been presented by independent algorithm in Visual‐infrared incident spectrum. We defined the range according to the retrieved results based on the analysis and comparison to many kinds of R‐R distribution function. The simulation computation results showed that the particles size measurement range is from 0.05 μm to 18 μm with incident spectrum from 0.4 μm to 2 μm and different refractive index. The results retrieved were satisfied even if 1 % noise was added into the backscattering intensity.     

Measurement of the resonant lengths of infrared dipole antennas

The resonant lengths of infrared dipole antennas at 10.6 and 3.39 μm are experimentally investigated. For this purpose, submicron-sized microbolometers coupled to dipole antennas with lengths between 0.7 and 20 μm were fabricated on a SiO₂-on-Si substrate. The response of the detector to 10.6 μm radiation shows a first resonance for an antenna length between 1.0 and 2.5 μm. A subsequent zero and a second attenuated resonance are observed as the antenna length increases. Similar behavior is observed for illumination at 3.39 μm, with a first resonance occurring at a length shorter than 1 μm. The results permit evaluation of an effective dielectric permittivity and shows the effect of the surface impedance of the metal on the propagation of current-wave on the antenna. The resonance behavior is further studied by changing the irradiation conditions of the detectors. Air-side and substrate-side illumination exhibit identical resonant antenna lengths, but different efficiencies of power collection. The antenna patterns as a function of incident angle have also been measured at 10.6 μm, showing a transition from a primary broadside lobe to the development of side lobes for longer antennas. Finally, an antenna response is measured at visible frequencies. Our measurements point out similarities, as well as differences, between infrared antennas and their counterparts at microwave frequencies, and provide insights useful for the design optimization of planar infrared antennas.     

SiC1-xGex/SiC 异质结光电二极管特性的研究

使用二维器件模拟软件Medici, 对SiC_1-xGe_x/SiC异质结的光电特性进行了模拟.设计了N型重掺杂SiC层的厚度为1 μm, P型轻掺杂SiC_1-xGe_x层厚为0.4 μm, 二者之间形成突变异质结.在反向偏压3 V、光强度为 0.23 W/cm²的条件下, p-n+ SiC_0.8Ge_0.2/SiC和p-n+ SiC_0.7Ge_0.3/SiC敏感波长λ分别可以达到0.64 μm和0.7 μm, 光电流分别为7.765×10^－7 A/μm和7.438×10^－7 A/μm; 为了进一步提高SiC_1-xGe_x/SiC 异质结的光电流, 我们把p-n+两层结构改进为p-i-n三层结构.在同样的偏压、光照条件下, p-i-n SiC_0.8Ge_0.2/SiC和p-i-n SiC_0.7Ge_0.3/SiC的光电流分别达到1.6734×10－6 A/μm和1.844×10－6 A/μm.     

深亚微米激光光刻研究

报道用远紫外准分子激光进行亚微光刻的实验结果，以波长为２４８．３ｎｍ的ＫｒＦ准分子激光为光源，以光管均匀器为主构成照明系统，采用带有平行平板为像差样正板的１：１折反射投影光刻物镜，在两种光刻胶上分别获得了０．６μｍ和０．５μｍ的光刻分辨率。     

通信用低损耗蜘蛛网结构包层空芯塑料布喇格光纤

提出并分析了利用蜘蛛网结构包层空芯布喇格光纤在0.65 μm~1.55 μm和200 μm ~500 μm波长范围得到低损耗传输的可能性.采用渐近转移矩阵公式所做的分析结果表明：这种光纤的传输损耗远低于构成光纤所用塑料的吸收损耗.在0.65 μm ~1.54 μm的可见至近红外波段,这种光纤结构可把构成光纤所用塑料的吸收损耗抑制为1/237 000,甚至可抑制为1/1 300 000;在200 μm ~500 μm的太赫兹波段,这种光纤结构可把构成光纤所用塑料的吸收损耗抑制为1/8 962,甚至可抑制为1/83 390.因此用便宜的塑料,可以在可见至太赫兹波段用这种光纤构成较长距离、较高带宽的光纤通信系统,并实现波分复用（WDM）.     

导弹尾烟对多波长激光传输影响研究

为研究1.06 μm、3.5 μm、10.6 μm三波长激光所受导弹推进剂尾烟干扰的差异程度,建立开放式烟道测试系统。在烟道头部放置装填有典型导弹推进剂的缩比发动机,点燃推进剂使之喷射并形成烟柱,在烟道尾部烟柱直径方向设置激光发射和接收装置,用以获取3波长的透过率。试验数据分析表明,烟雾对激光的衰减与烟雾粒子半径有关,在400 m烟道长度环境中, 10.6 μm激光透过率最高可达1.06 μm激光的104倍。该结果有益于激光制导武器的改进和升级。     

合肥光源束流闭轨局部调整和校正

 针对特定实验站调整光源点位置的要求,设计了合肥光源储存环束流闭轨局部调整和校正系统,介绍了该系统的工作原理、硬件组成、软件设计及运行结果,设计要求束流闭轨局部调整的最大幅度为1~2 mm,水平方向和垂直方向其余闭轨畸变均方根分别小于50和30 μm。校正系统采用轨道设定法作为束流闭轨局部调整和校正算法,由束流轨道测量系统、校正铁系统和控制系统组成。运行结果显示：水平和垂直方向分别调节2.0和1.5 mm,水平方向和垂直方向其余闭轨畸变均方根分别为45.14和27.62 μm。