PN结对交流信号相位的影响(续)

当1个交流小信号被1个PN结和1个大电容分压,且该电容的电容值远大于PN结电容时,大电容两端的电压与PN结电容成正比,该信号的相位与PN结的电阻以及信号的频率有关.把PN结当作1个电容和1个电阻并联,可定性解释该信号的相位与PN结正向电阻、与加在PN结两端的直流反向偏压、在零直流偏压下与交流信号频率的关系.     

PN结正向伏安特性曲线随温度的变化

介绍了在不同温度下，PN结正向伏安特性曲线的自动测量方法。讨论了PN结伏安特性与温度的关系．由于正向结电压小于内建电势差，温度升高或正向结电压增加，正向结电流将增大，温度升高反向结电流也相应增加．当温度趋向OK时。正向结电压趋向内建电势差。     

PN结对交流信号相位的影响

交流小信号被PN结和电容分压，且电容值远远大于PN结电容值时，大电容两端的电压是很小的交变电压，该信号的相位与PN结的内阻(正向)有关．把PN结当做一个电容和一个电阻并联，可定性解释这种关系．     

应用计算机测定PN结正向压降的温度特性

采用电热法把待测的PN结放置于温度可连续变化的热源中,利用精确的温度传感器进行温度测量,并利用计算机数据采集技术,直观地再现了PN结正向压降随温度线性变化的整个物理过程,提高了测量的精度.     

Measurement of the total absorption coefficient of a KTP crystal

The laser calorimetric measurement of the absorption coefficient in a small cubic 12 × 9 × 9 mm KTP crystal has been investigated experimentally. The absorption coefficient in this crystal is 0.0121 cm^-1, and the measurement accuracy is within 10%.     

标定水汽吸收系数的实验研究

利用吸收光谱方法检测水汽含量的精确度主要取决于水的吸收系数标定. 采用露点法对气瓶的水汽含量进行了精确测定,并将气瓶中气体通入测试池,通过改变测试池中气体的压力来改变水汽分压,从而实现了水汽吸收系数的标定,标定结果为水汽单位长度的吸收系数为8.6×10-3/Pa·m.     

光吸收介质的吸收系数与介电函数虚部的关系

讨论了相对介电函数虚部和消光系数与光吸收的关系,指出吸收系数与消光系数成正比,而吸收系数与相对介电函数虚部成正比是有条件的.     

硅的间接跃迁双光子吸收系数谱

利用皮秒Nd:YAG脉冲激光器作为激发光源,测量出光子能量介于1.36 μm (0.912 eV)—1.80 μm (0.689 eV)之间的硅间接跃迁双光子吸收系数谱.尽管此波段范围内的激光光子能量小于硅间接带隙,但当激光辐照在硅基光电二极管受光面时,在二极管两电极端仍然探测到了显著的脉冲光伏信号.光伏信号峰值强度与入射光强呈二次幂函数关系,表明其是双光子吸收过程.采用pn结等效结电容充放电模型,将光伏响应信号峰值与入射光强相关联,从中提取出硅的间接跃迁双光子吸收系数,改变入射波长得到系数谱.研究表明:     

Enhanced absorption process in the thin active region of GaAs based p–i–n structure

The optical absorption is the most important macroscopic process to characterize the microscopic optical transition in the semiconductor materials. Recently, great enhancement has been observed in the absorption of the active region within a p–n junction. In this paper, Ga As based p–i–n samples with the active region varied from 100 nm to 3 μm were fabricated and it was observed that the external quantum efficiencies are higher than the typical results, indicating a new mechanism beyond the established theories. We proposed a theoretical model about the abnormal optical absorption process in the active region within a strong electric field, which might provide new theories for the design of the solar cells,photodetectors, and other photoelectric devices.     

Trends in the spectral distribution of the absorption coefficient of complex organic molecules

General trends in formation of the observed vibrational spectra are analyzed by calculating spectral distributions of the absorption coefficient in the IR region for 45 molecules of different classes ignoring the electrooptical paramaters of particular bonds and structural groups. It is shown that for many molecules, only vibrations of peripheral X-H bonds make a prevailing contribution to the total integral absorption in a wide spectral range. The effect of increasing intensities of some bands is clearly observed for skeleton vibrations, when optical parameters of external X-H bonds are zero. V. I. Vernadski Institute of Geochemistry and Analytical Chemistry of the Russian Academy of Sciences, 19, Kosygin St., Moscow, 117975, Russia. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 65, No. 4, pp. 491–496, July–August, 1998.     

大气气溶胶粒子光吸收系数的测量

采用核孔过滤膜累积气溶胶粒子的方法设计了气溶胶粒子光吸收系数的测量系统。该系统由双光路组成,可以减小光路损耗和电路噪声带来的各种测量误差。同时,具有体积小、光路易于调节、可进行实时测量、定标容易等特点。用200和400nm孔径的过滤膜,分别测量了实验室内大气气溶胶粒子对不同波长激光的吸收系数。随着累积时间的增加,系统的测量精度也不断的提高,在累积时间为900s时,系统测量误差为9.849×10-6/m。     

Two-photon absorption coefficient in relation to the typical pulse models of laser

The two-photon absorption (TPA) coefficient (β) relating to pulse models of laser is theoretically studied based on the nonlinear absorption equation. An expression of nonlinear energy transmission is obtained, in which a factor (g) is introduced to describe the β deviation resulting from the pulse profile of laser. The relative deviation can be then expressed as (1/g − 1)% for comparing β obtained based on other pulse models of laser with β₀ based on the rectangular one. The values of g factor and the deviation of some typical ultra-short pulse models used nowadays are also calculated and presented. Our results suggest that the β deviations from the temporal pulse shapes should not be neglected in usual nonlinear transmission measurement. The g factor may become a useful parameter in taking account of this deviation.     

采用光热辐射计量术测量固体材料的光谱吸收系数

本文采用一种新的测试技术——光热辐射计量术(PTh),对固体材料进行非接触式光谱研究,文中介绍了光热辐射计量理论,并在实验上获得Ce_2O_3粉末和果树叶的相对光谱吸收系数.     

MATLAB拟合工具箱在PN结物理特性综合实验中的应用

介绍了PN结物理特性综合实验原理,利用绘图软件Matlab对实验数据进行曲线拟合,得到了PN结伏安特性函数表达式和PN结正向压降与温度间关系的拟合曲线,计算了常温下玻尔兹曼常数和PN结温度传感器灵敏度及T=0 K时的半导体近似禁带宽度。     

Measurement of the optical absorption coefficient for liquid based on optical microfiber

An inline measuring method of the optical absorption coefficient for liquid based on optical microfiber (OM) is studied. If an OM is immersed into absorptive liquid, the additional loss of the OM will increase. We have analyzed the relationship between the additional loss of the OMs and the absorption coefficients of the liquids, and found that the OM with determinate construction will be useful for measuring the absorption coefficients of the liquid whose refractive index is lower than that of the OM. Two OM samples are prepared to measure the absorption coefficient of pure water. A supercontinuum source is launched into the OM sample which is immersed into pure water, and absorption spectrum from 1400 to 1700 nm has been achieved by monitoring the additional loss. The trend of the absorption spectrum is similar with that of the reported result, showing that the inline measurement of the optical absorption coefficient is a feasible method for those lower refractive index liquids.     

PN结伏安特性的实验研究

介绍了验证PN结伏安关系特性实验的实验原理,并利用绘图软件Origin7.5对实验数据进行处理.结果表明,PN结的扩散电流和两端的正向电压之间满足指数关系.通过与理论公式的比较,准确地测出了玻尔兹曼常数.     

声学覆盖层吸声系数的多通道逆滤波测量

提出了一种利用最小二乘求逆计算的声学覆盖层吸声系数多通道逆滤波测量方法.该方法通过估计电路信道及水声信道的信道响应,利用最小二乘实现多通道逆滤波算法,通过多路逆信号的同步发射在声学覆盖层处实现高分辨率主瓣、低旁瓣和时域窄脉宽的入射波聚焦,从而提高声学覆盖层低频吸声系数的测量精度。仿真验证了该方法在混响抑制和空时聚焦中的效果.在压力水罐中进行了频率为0.8~5 kHz条件下的钢板试样反射系数和透射系数的测量实验,通过与理论计算值对比,验证了该测量方法的有效性。论文提出的方法适用于非自由场环境下声学覆盖层吸声系数的测量,尤其适用于低频条件下吸声系数的测量。     

银吸收边附近X射线衰减系数测量

在北京同步辐射装置的4B7A中能X光束线上,光源能区为2.1~6.0keV,能量分辨大于5000,高次谐波小于0.1%,光源强度大于109光子/s。通过全能区多能点的透过率精确测量Ag样品质量厚度,然后采用Ag薄膜对单能X光子的透过率进行测量,给出了Ag薄膜在吸收边(3.4~3.9keV)的衰减系数。建立了Ag样品吸收边附近衰减系数同步辐射测量方法。通过不确定度分析给出衰减系数测量不确定度小于1%,填补了在该区间衰减系数的空白。     

银吸收边附近X射线衰减系数测量

在北京同步辐射装置的4B7A中能X光束线上,光源能区为2.1~6.0 keV,能量分辨大于5000,高次谐波小于0.1%,光源强度大于109光子/s。通过全能区多能点的透过率精确测量Ag样品质量厚度,然后采用Ag薄膜对单能X光子的透过率进行测量,给出了Ag薄膜在吸收边（3.4~3.9 keV）的衰减系数 。建立了Ag样品吸收边附近衰减系数同步辐射测量方法。通过不确定度分析给出衰减系数测量不确定度小于1％,填补了在该区间衰减系数的空白。     

内混合气溶胶粒子体系有效吸收系数的计算

分析了以黑碳和水组成的内混合强吸收气溶胶粒子体系有效吸收系数随时间变化的规律,并讨论了不同波长、不同半径比等对有效吸收系数的影响。结果表明：波长越短,内混合气溶胶粒子体系有效吸收系数越大,在1~100 s内随时间增大的速度也越快,1~100 s内的增幅比100~1000 s内的大,最大增幅达到132.65%;不同的内外半径比对内混合气溶胶粒子体系的有效吸收系数有较大影响,内外半径比越大,有效吸收系数越大,在1~100 s有效吸收系数增加速度越快,1~100 s内增幅较大,最大增幅达到138.66%。