高精度虹膜识别光学镜头的研制

针对虹膜识别系统中难于获取高分辨率的虹膜图像问题,设计一款高精度虹膜图像采集摄像镜头。镜头焦距14.2 mm, 畸变小于0.15%,像方数值孔径为0.26,像面直径为5.35 mm,工作距离130 mm,物像共轭距为150 mm。光学系统可获得高分辨率图像,在0.7视场光学传递函数MTF在120 lp/mm时大于30%。镜头由4片球面透镜构成,结构简单,适合产业化生产,各项光学指标检测结果达到设计要求。     

STUDY OF OPTICAL PUMPING OF ALKALI ATOMIC BEAM IN STRONG MAGNETIC FIELDS

We have gained a very comprehensive set of results for infrared diffraction (10.6μm wavelength) from fabricated single grooves of reflection with widths in the range of 5μm to 65μm. The experimental results show that the diffraction can still occur when the groove width becomes comparable to or less than the wavelength of the probing light. Variations of the diffraction intensities have a very regular sinusoidal relationship with the polarization angle of the incident light; and the diffraction intensities are the when the incident light is TM polarized. However, the diffraction intensities will be a minimum when the incident light is TE polarized; and the biger the diffraction angle, the higher the rate of change of the diffractive intensity with increasing polarization angle of the incident light.     

镶嵌于基质中的金属超微粒子特性研究(Ⅰ)——超微粒子的量子阱点模型

提出超微粒子(UFP)的量子阱点模型。模型假定UFP的主要特性由其非定域电子(简称电子)决定,电子被束缚在三维有限深势阱内。电子的行为由二部分组成:单电子的和集体化的。电子能谱主要由单电子行为决定。模型反映了UFP的一些重要特性,例如块体材料逸出功,UFP原子半径和第一电离能,而忽略UFP更精细的结构。这种近似被证明是合理的。一系列有用的公式和预言被导出。(1)主要的UFP特性,量子尺寸效应和电子能谱的壳层结构。(2)UFP的逸出功和费密能级公式,这对于其他模型是困难的。导出的UFP逸出功随尺寸变化的公式 关键词：     

无标样X射线定量分析最小二乘法方程的稳定解

无标样法是X射线定量分析的重要方法。无标样定量联立方程中经常出现的病态方程使定量结果出现很大的误差。最小二乘法方程组在某些组合情况下也会出现严重的病态方程。本文提出可以获得可靠的稳定解的无标样X射线定量最小二乘法。指出不同样品数及组合条件下获得稳定解的计算方法:直接最小二乘法、算术平均法、稳定性因子判别法。 关键词：     

The beam-based calibration of an X-ray pinhole camera at SSRF

A pinhole camera for imaging X-ray synchrotron radiation from a dipole magnet is now in operation at the Shanghai Synchrotron Radiation Facility (SSRF) storage ring. The electron beam size is derived by unfolding the radiation image and the point spread function (PSF) with deconvolution techniques. The performance of the pinhole is determined by the accuracy of the PSF measurement. This article will focus on a beam-based calibration scheme to measure the PSF system by varying the beam images with different quadrupole settings and fitting them with the corresponding theoretical beam sizes. Applying this method at SSRF, the PSF value of the pinhole is revised from 37 to 44 μm. The deviation in beam size between the theoretical value and the measured value is minimized to 4% after calibration. This optimization allows us to observe the horizontal disturbance due to injection down to as small as 0.5 μm.     

阴极荧光光谱有效收集效率的计算与测量（I）

从点光源均匀发光模型出发,重点导出了回转半椭球面镜的阴极荧光(Cathodoluminescence,简称CL)光谱有效收集效率η_λ~(eff)的计算公式,分析讨论了收集效率η_λ~(eff)与椭球参数e、收集角、Δφ出射角Δ(?)以及出射光束方位角θ_N的关系,给出了相应的理论计算和模拟实验结果.研究表明,理论计算与实验结果一致.     

荧光光度法测定雨水中的H2O2含量

研究了在pH4.48的HAc-NaAc缓冲溶液中,邻苯二胺(OPDA)与过氧化氢反应生成新物质2,3-二氨基吩嗪(DAPN)的荧光光谱变化,通过跟踪DAPN的荧光强度建立了过氧化氢测定的新方法,该方法由于采用二元体系,实验操作简单,灵敏度较高。实验结果表明,过氧化氢含量在9.0×10-7～3.6×10-5mol.L-1范围内与荧光强度的变化呈良好的线性关系,线性方程为:F=1.15c(μmol.L-1) 398.6,相关系数r=0.9991,最低检出限为2.7×10-7mol.L-1(3Ds/斜率,n=11)。对含量为7.5×10-6mol.L-1和3.0×10-5mol.L-1的H2O2的标准溶液进行了11次平行测定,其相对标准偏差分别为2.2%和1.0%。考察了多种共存离子的影响。该方法用于雨水中微量H2O2的测定,测定结果令人满意。     

圣诞树底座灯系统的光学参数对照测量与数据分析

某公司生产的圣诞树由于质量问题在销往国外时被烧毁。采用故障样品和参照样品比较测量法,在同等条件下,分别测量两个样品的光谱辐射照度分布,波段积分辐射照度,色温,以及温度特性等参数。实验结果表明:故障样品与参照样品的色温分别为2722K和3060K。在紫外波段、可见波段和近红外波段,故障样品的积分辐射照度分别是正常样品的1.7倍、2.4倍和10.7倍。故障样品的灯系统未进行任何技术处理,而参照样品的灯系统进行了可见与近红外吸收处理,因此总辐射照度显著减弱。温度特性实验结果表明:在同样的受辐照时间7min内,故障样品的温升高达101.5℃,而参照样品的温升只有46.4℃。这些参数的差异可能是导致圣诞树烧毁的主要原因。     

固体吸附管捕集冷原子吸收光谱法测定工作场所空气中汞的研究

建立了工作场所空气中汞及其化合物的高锰酸钾-二氧化锰混合固体吸附管捕集、冷原子吸收测定方法。用高锰酸钾与二氧化锰按质量比1∶1混合后填装玻璃管制成固体吸附管捕集工作场所空气中汞,并以0.90 mol·L-1的硫酸溶液解吸后冷原子吸收光谱法测定,与高锰酸钾-硫酸吸收液法的采样效率、样品稳定性、穿透容量进行了比对。在0.000 2~0.015 0 mg·L-1的浓度范围内线性关系良好,相关系数为0.999 1,空气中汞在0.001~2.820 mg·m-3范围内,平均采样效率为99.9%~100.0%,300 mg吸附剂对汞的穿透容量大于505.4 μg,吸附管对汞的平均加标回收率为96.4%~103.8%,日内、日间精密度分别为3.0%~3.3%,3.5%~5.2%,最低检出浓度为0.001 3 mg·m-3(以采集7.5 L空气样品计)、0.000 6(以96 L空气样品计)。采集后的吸附管在室温下保存30 d,下降率小于0.1%。固体吸附管采样方法简单,适用于工作场所空气中汞及其化合物的短时间、时间加权平均浓度及个体暴露浓度的采样检测。     

An Easily Switchable Dual-Wavelength Passively Mode-Locked Erbium Fiber Laser

A simple scheme of switchable dual-wavelength passively mode-locked fiber laser is demonstrated. The laser can be flexibly switched among different mode-locked states simply by tuning the cavity loss while keeping all the other cavity parameters fixed. As the cavity loss increases, the mode-locked fiber laser operates at the long-wavelength, dual-wavelength, and short-wavelength states, successively. In addition, these states can be conveniently switched without losing the mode-locked operation and the switching process is reversible as the cavity loss decreases. The mechanism is qualitatively explained by the balance between the fiber gain and the cavity loss.