球形光纤端面效应及其应用

本文介绍了球形光纤端面的制作方法,采用射线理论和等效透镜法分析了圆球形端面多模光纤的端面效应,并给出了两个不同端面多模光纤之间耦合的实验结果。结果表明：圆球形端面光纤具有聚光特性,与平端面相比,使用圆球形端面光纤不仅可以提高光器件之间的耦合效率,而且增大了它们之间的耦合距离,利于光路调试;可广泛应用于光源与光纤、光纤与光纤、光纤与探测器之间的耦合。     

The Monte-Carlo simulation on a scintillator neutron detector

A simulation of the properties of the shifting scintillator neutron detector using 6LiF/ZnS(Ag) scintillation screens is performed.The simulation results show that the light attenuation length of standard BC704 scintillator is about 0.65 mm.Its thermal neutron detection efficiency,gamma sensitivity and intrinsic spatial resolution can achieve around 50.0%,10 5and 0.18 mm(along X-axis) respectively.For the detector,air coupling position resolution is better than the silicone oil coupling.Some of the simulation results are compared with experimental results.They are in agreement.This work will be helpful for constructing neutron detector for high intensity powder diffractometer at Chinese spallation neutron source.     

风云二号辐射计百叶窗式遮光罩杂散光抑制研究

风云二号卫星扫描辐射计为视场分光方式的R-C光学系统,视场外的杂光掠过次镜穿过主镜孔直接混入信号光路照射在焦面上,形成直射杂光。为了消除该直射杂光,使用TracePro软件对辐射计模型进行正追和倒追,都追到了直射杂光的存在,利用Zemax软件仿真找出了该直射杂光的形成机理,并计算出该直射杂光域。根据仿真和计算,设计了可以透信号光阻挡杂散光的叶片状次镜遮光罩。软件仿真表明:百叶窗式遮光罩可以彻底抑制该区域可见直射杂光,积分球实验也验证了该百叶窗式遮光罩可以降低辐射计95.2%的可见杂光。     

一种微波光子探测器组件的封装设计与实现

为实现微波光子系统的高集成度、高可靠性,进行了一种微波光子探测器组件的封装设计与实现。介绍了定制化封装设计思路,选择可伐合金作为壳体材料,采用的卧式贴装方案中选用斜面透镜光纤,给出了封装工艺流程和关键工艺点,最终封装的组件光电耦合效率在68%～79%之间,满足总体指标需求。该组件通过混合集成封装方法,实现了微波芯片与光子芯片在同一封装内的阵列化集成及气密性封装。该组件的封装设计与实现方法,可用于其他微波光子产品,有助于提升光载射频传输系统的集成度与可靠性。     

神光Ⅲ原型受激拉曼与受激布里渊散射份额测量

激光注入率测量是黑腔耦合效率测量至关重要的一个环节,主要通过散射光测量来实现。在神光Ⅲ原型激光装置上进行的黑腔物理实验中,利用PIN探头阵列进行了散射光角分布测量。通过拟合分析,发现原型装置上激光等离子体非线性相互作用较神光Ⅱ装置要强,其中受激拉曼份额在10%量级,受激布里渊散射在20%量级。将由此评估的激光靶耦合效率代入辐射温度定标率公式中,得出的辐射温度值与实验中Dante测量值符合较好,说明对参量过程份额的评估具有一定可靠性。     

神光Ⅲ原型受激拉曼与受激布里渊散射份额测量

激光注入率测量是黑腔耦合效率测量至关重要的一个环节,主要通过散射光测量来实现。在神光Ⅲ原型激光装置上进行的黑腔物理实验中,利用PIN探头阵列进行了散射光角分布测量。通过拟合分析,发现原型装置上激光等离子体非线性相互作用较神光Ⅱ装置要强,其中受激拉曼份额在10%量级,受激布里渊散射在20%量级。将由此评估的激光靶耦合效率代入辐射温度定标率公式中,得出的辐射温度值与实验中Dante测量值符合较好,说明对参量过程份额的评估具有一定可靠性。     

光强局部选通成像器中光锥耦合技术研究

为了实现景物在强光照射下能够分辨图像的细节,在液晶的光强局部选通成像器中,使用光锥将TFT-LCD液晶耦合到CCD相机上以实现图像的实时传递。通过理论分析和计算,采用光锥耦合获得的耦合效率为14.24%,而透镜耦合则只有1.83%,由前者耦合后构成的局部选通系统,其调制传递函数曲线中奈奎斯特频率为0.518,极限分辨率为34 lp/mm,由此制作的器件,在对高照度下图像的细节分辨,明显高于透镜耦合的器件。分析了造成该系统MTF下降的因素,并提出了进一步改善MTF的技术措施。     

Performance of superconducting nanowire single-photon detector with the fan coupling antenna array

The performance of superconducting nanowire single-photon detector （SNSPD） involving niobium nitride with the fan coupling antenna array is analyzed. The SNSPD has a high detection efficiency and counting rate. Hydrogen silsesquioxane and niobium nitride are filled in the gold grating deposited on the substrate in which the fan coupling antenna arrays are embedded. By changing the position of the fan coupling antenna array, the maximum area of optical intensity is obtained and the photon collection efficiency is increased by 26.5 times. The detection efficiency of SNSPD is improved without changing the detection speed. These parameters are important for designing a practical single-photon detector,     

Integration of a field-effect-transistor terahertz detector with a diagonal horn antenna

Efficient coupling of terahertz electromagnetic wave with the active region in a terahertz detector is required to enhance the optical sensitivity. In this work, we demonstrate direct integration of a field-effect-transistor(FET) terahertz detector chip at the waveguide port of a horn antenna. Although the integration without a proper backshot is rather preliminary, the noise-equivalent power is greatly reduced from 2.7 nW/Hz~(1/2) for the bare detector chip to 76 pW/Hz~(1/2) at340 GHz. The enhancement factor of about 30 is confirmed by simulations revealing the effective increase in the energy flux density seen by the detector. The simulation further confirms the frequency response of the horn antenna and the onchip antennas. A design with the detector chip fully embedded within a waveguide cavity could be made to further enhance the coupling efficiency.     

应用于红外跟踪系统的光纤耦合技术

本文介绍了一种解决红外跟踪系统中探测器和致冷器组件位于万向支架机构上各种弊病的方法。利用纤维光束的柔软性，应用光纤耦合技术，可以让探测器和致冷器组件放在离万向支架一定距离上。文中着重论述了光纤与探测器间的光耦合问题，并就一组合透镜耦合方案作了具体设计计算。最后谈了谈光纤耦合技术研究的总体思路和对以后工作的设想。     

RIBLL终端大面积中子探测器阵列研制方案的理论计算

介绍了一种用于丰中子核研究的RIBLL终端大面积中子探测器阵列的研制.利用Geant4软件包对该探测系统的中子探测效率、时间分辨和位置分布等进行了蒙特卡罗模拟,同时对探测器的cross?talk进行了研究.给出了探测器的设计方案.     

THzQWP二维光栅耦合效率的理论分析研究

将二维金属光栅结构引入到探测器结构中,以提高太赫兹(THz)量子阱光电探测器的探测率。采用三维时域有限差分算法,建立了THz量子阱光电探测器的二维金属光栅仿真模型,详细分析了二维金属光栅参数对太赫兹量子阱光电探测器的电场强度的影响。仿真分析结果表明:当入射光频率为6.27 THz(相对应波长为47.847 m)、光栅周期P=10.5 m、占空比=0.55（金属块宽度w= 5.755 m）、光栅层厚度h=0.4 m时,器件中的Z方向上的电场值最大,光栅的耦合效率最高。     

工业CT光电二极管探测器灵敏度

在工业CT系统设计过程中,射线能量选择、探测器结构设计、射线源和探测器匹配等方面都涉及探测器灵敏度问题。研究了影响工业CT光电二极管探测器灵敏度的几个主要因素及其定量关系。首先分析了灵敏度的几个主要影响因素：能量沉积率、绝对闪烁效率、光收集效率、光电转换效率。然后采用蒙特卡罗方法仿真得到闪烁体的能量沉积率、光收集效率,计算了CsI(Tl)闪烁体的荧光转换效率及光电二极管的光电转换效率,定义了闪烁体与光电二极管的匹配度的概念。最后得出具有普遍意义的探测器灵敏度的表达式,理论计算值与实际测量结果最大相差20.4%,实验验证了该灵敏度计算方法的有效性和正确性。     

工业CT光电二极管探测器灵敏度

在工业CT系统设计过程中,射线能量选择、探测器结构设计、射线源和探测器匹配等方面都涉及探测器灵敏度问题。研究了影响工业CT光电二极管探测器灵敏度的几个主要因素及其定量关系。首先分析了灵敏度的几个主要影响因素:能量沉积率、绝对闪烁效率、光收集效率、光电转换效率。然后采用蒙特卡罗方法仿真得到闪烁体的能量沉积率、光收集效率,计算了CsI(Tl)闪烁体的荧光转换效率及光电二极管的光电转换效率,定义了闪烁体与光电二极管的匹配度的概念。最后得出具有普遍意义的探测器灵敏度的表达式,理论计算值与实际测量结果最大相差20.4%,实验验证了该灵敏度计算方法的有效性和正确性。     

波导与探测器吸收层垂直耦合结构中的光学耦合分析

利用几何学理论分析了波导与探测器吸收层之间的光学传播情况，以硅基波导与ＧｅＳｉ／Ｓｉ多量子阱ＰＩＮ探测器吸收层主分析对象，说明光学耦合效率与两层介质的折射率分布及吸收层长度的关系。     

盲优化波前校正提高自由空间光通信光纤耦合效率

为了提高自由空间光通信系统的光纤耦合效率,介绍了一种新颖的基于盲优化波前校正的自适应光学系统。该系统不使用波前传感器,而是在信号进入接收端前,将畸变光信号分束后送入光电探测器,进行耦合效率计算;采用耦合效率的估计公式斯特列尔比为目标函数,用随机并行梯度优化算法最大化目标函数,以实时控制变形镜,从而使耦合进入单模光纤的光达到最优。数值结果表明,此系统能使光纤耦合效率从6%提高到约60%。     

盲优化波前校正提高自由空间光通信光纤耦合效率

为了提高自由空间光通信系统的光纤耦合效率,介绍了一种新颖的基于盲优化波前校正的自适应光学系统。该系统不使用波前传感器,而是在信号进入接收端前,将畸变光信号分束后送入光电探测器,进行耦合效率计算;采用耦合效率的估计公式斯特列尔比为目标函数,用随机并行梯度优化算法最大化目标函数,以实时控制变形镜,从而使耦合进入单模光纤的光达到最优。数值结果表明,此系统能使光纤耦合效率从6%提高到约60%。     

NE213 闪烁体探测器中子探测效率模拟

应用FLUKA 软件包对NE213 液体闪烁体中子探测器的探测效率进行了蒙特卡罗模拟,通过Birks 公式将中子产生的次级粒子的能量沉积转化为相应的光输出。根据不同探测阈值对模拟得到的光输出进行积分处理,计算出给定能量下探测器的中子探测效率。将模拟得到的闪烁体光输出、中心探测效率和平均探测效率随中子入射到探测器前表面位置的变化与实验数据进行比较,结果显示,FLUKA 模拟结果与实验值符合得很好,这为中子探测器的设计提供了可靠保证。A NE213 liquid scintillation neutron detector was simulated by using the FLUKA code. The light output of the detector was obtained by transforming the secondary particles energy deposition using Birks formula. According to the measurement threshold, detection efficiencies can be calculated by integrating the light output. The light output, central efficiency and the average efficiency as a function of the front surface radius of the detector, were simulated and the results agreed well with experimental results.     

Four-band quantum well infrared photodetector array

A four-band quantum well infrared photodetector (QWIP) focal plane array (FPA) has been demonstrated by stacking different multi-quantum well structures, which are sensitive in 4–5.5, 8.5–10, 10–12, and 13–15.5 μm infrared bands. This 640 × 514 format FPA consists of four 640 × 128 pixel areas which are capable of acquiring images in these infrared bands. In this application, instead of quarter wevelength groove depth grating reflectors, three-quarter wavelength groove depth reflectors were used to couple radiation to each QWIP layer. This technique allows us to optimize the light coupling to each QWIP stack at corresponding pixels while keeping the pixel (or mesa) height at the same level, which will be essential for indium bump-bonding with the multiplexer. In addition to light coupling, these gratings serve as a contact to the active stack while shorting the unwanted stacks. Flexible QWIP design parameters, such as well width, barrier thickness, doping density, and the number of periods, were cleverly exploited to optimize the performance of each detector while accommodating requirements set by the deep groove light coupling gratings. For imaging, detector array is operated at temperature T=45 K, and each detector shows a very high D^*>1×10¹¹ cm  /W for 300 K background with f/2 optics. This initial array gave excellent images with 99.9% of the pixels working, demonstrating the high yield of GaAs technology.     

Low frequency characteristics of a quasioptical Schottky diode detector part II: Experimental results

A detailed experimental study of the low frequency (video) response of a quasioptical Schottky diode detector over the microwave and FIR wavelength range is presented. An optimization of the responsivity versus the bias current is proposed and a generalized curve of the saturation power versus the FIR wavelength is given. This curve defines for any antenna point-contact Schottky diode detector, suitable for FIR detection, the power range for a linear detector response. A simple method is also described to calculate the coupling efficiency of the laser radiation into the antenna reception pattern.