共查询到18条相似文献,搜索用时 156 毫秒
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EBCCD的增益及信噪比研究 总被引:7,自引:0,他引:7
以背照明减薄CCD为基础的微光成像系统 ,可以得到视频信号速率的输出。这种减薄的电子轰击CCD探测系统 (EBCCD)在微光下的性能大大超过了像增强器耦合的CCD探测系统 (ICCD)。EBCCD能在微光条件下产生高对比度、高分辨力的视频信号。可以预料 ,它将在工业应用、军事应用及科学研究工作中取代通常使用的ICCD。详细讨论了影响EBCCD的增益及信噪比的各种因素。结果表明 ,若适当提高阴极和CCD之间的电压 ,减小CCD基片的厚度 ,可以进一步减小EBCCD的噪声 ,从而使信噪比得到更大的提高 相似文献
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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。 相似文献
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利用微光像增强器的图像增强功能,将微光像增强管耦合到电荷耦合器件(CCD)上即构成微光图像增强CCD(简称ICCD)。它具有两个重要的特性:一是通过选择适当的像管输入窗及光电阴极,使ICCD光谱响应范围由可见光扩展到X射线、紫外、近红外区域,从而使该器件能适用于各种用途;二是使ICCD的灵敏度达到10-4lx以下,实现了ICCD摄像器件在黎明或黄昏的照度下(102lx)在1/4月光下(10-2lx)、在星光下(10-4lx)都能有效的工作。微光ICCD电视摄像系统可应用在天文、医疗、火控、制导、飞机紫外预警等方面。重点阐述了微光ICCD电视摄像技术的发展与性能评价。 相似文献
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《光子学报》2010,(Z1)
分辨力和信噪比是像增强型CCD成像系统的两个最主要的参量.为了分析CCD相机分辨力对像增强型CCD成像系统分辨力的影响,本文分别用一个高分辨力像增强型CCD相机和一个普通分辨力CCD相机分别与相同的中继透镜、像增强器和前置镜头耦合,得到一套高分辨力像增强型CCD实验样机和一套对比像增强型CCD实验样机;在不同照度下测量了两套实验样机的分辨力和信噪比,实验结果分析表明:当照度高于1.84×10-3 lx时,像增强型CCD成像系统分辨力受器件分辨力和信噪比共同影响,高分辨力像增强型CCD实验样机分辨力要高于对比像增强型CCD实验样机分辨力.当照度低于1.84×10-3 lx时,像增强型CCD成像系统分辨力主要受器件信噪比的影响,高分辨力像增强型CCD实验样机与对比像增强型CCD实验样机分辨力相当. 相似文献
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为了实现在较低剂量下获得较高的分辨率,研制了一款价格低廉的X射线CCD相机。该相机使用硫氧化钆作为转换屏、经一代像增强器增强后的图像通过光锥耦合到CCD相机上;为了提高系统的光传输效率,提出了将像增强器输出直面板或倒像器直接更换成光锥,其小端直接同CCD相机耦合的方案;通过灰度分析计算对比度曲线,拟合得出系统的本征空间分辨率为13 Lp/mm;通过拍摄实际景物,可以清晰地看到其内部的细节,显示出比较好的图像质量。 相似文献
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An acrylic-based Y-branch plastic optical fiber (POF) with a middle suspended waveguide taper has been developed. The suspended
high index contrast waveguide taper structure has been designed in such a way that it is surrounded by air-cladding. Non-sequential
ray tracing has been performed on the device giving an insertion loss of 4.68 dB and coupling ratio of 50: 50. The middle
waveguide taper is constructed on the acrylic block itself without using any additional optical waveguiding medium injected
into the engraved taper region. Fabrication of the devices is done by producing the device structures on an acrylic block
using high speed computer numerical control (CNC) machining tool. Input and output POF fibers are inserted into this device
structure in such a way that they are passively aligned to the middle waveguide taper structure. The device shows an insertion
loss of 5.9 dB, excess loss of 2.9 dB and a splitting ratio of 50: 50. 相似文献
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We proposed a simple low-cost acrylic and metal-based Y-branch plastic optical fiber (POF) splitter which utilizes a low cost optical polymer glue NOA63 as the main waveguiding medium at the waveguide taper region. The device is composed of three sections: an input POF waveguide, a middle waveguide taper region and output POF waveguides. A desktop high speed CNC engraver is utilized to produce the mold inserts used for the optical devices. Short POF fibers are inserted into the engraved slots at the input and output ports. UV curable optical polymer glue NOA63 is injected into the waveguide taper region and cured. The assembling is completed when the top plate is positioned to enclose the device structure and connecting screws are secured. Both POF splitters have an average insertion loss of 7.8 dB, coupling ratio of 55: 45 and 57: 43 for the acrylic and metal-based splitters respectively. The devices have excess loss of 4.82 and 4.73 dB for the acrylic and metal-based splitters respectively. 相似文献
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We proposed a simple low-cost acrylic and metal-based Y-branch plastic optical fiber (POF) splitter which utilizes a low cost
optical polymer glue NOA63 as the main waveguiding medium at the waveguide taper region. The device is composed of three sections:
an input POF waveguide, a middle waveguide taper region and output POF waveguides. A desktop high speed CNC engraver is utilized
to produce the mold inserts used for the optical devices. Short POF fibers are inserted into the engraved slots at the input
and output ports. UV curable optical polymer glue NOA63 is injected into the waveguide taper region and cured. The assembling
is completed when the top plate is positioned to enclose the device structure and connecting screws are secured. Both POF
splitters have an average insertion loss of 7.8 dB, coupling ratio of 55: 45 and 57: 43 for the acrylic and metal-based splitters
respectively. The devices have excess loss of 4.82 and 4.73 dB for the acrylic and metal-based splitters respectively. 相似文献
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We report a novel scheme to build a compact, tunable fiber laser. The tuning mechanism is based on the transmission property of a single-mode biconic fiber taper. While pulling the taper, we observe oscillations in the transmitted optical power that are due primarily to interference between a pair of excited modes within the tapered region, which are eventually coupled into the unstretched single-mode fiber at the end of the taper. A similar mechanism causes the modulation of the transmitted optical spectrum after the taper has been pulled and stabilized. It is this spectral modulation by the taper that is exploited here to control the wavelength of a fiber laser. The modulation can be adjusted by stretching the taper, thus enabling the tuning of the laser wavelength. We have built a 32 mW Er-doped tunable ring fiber laser with a continuous tuning range of over 20 nm and a signal-to-noise ratio of better than 45 dB over the entire tuning range; our output power is limited only by the available pump power. 相似文献