共查询到16条相似文献,搜索用时 125 毫秒
1.
根据建立的变掺杂变组分反射式AlxGa1–x As/GaAs光电阴极的分辨力模型以及调制传递函数(MTF)理论模型,仿真了材料中掺杂浓度线性变化、Al组分线性变化,掺杂浓度均匀不变、Al组分线性变化,掺杂浓度线性变化、Al组分均匀不变,掺杂浓度均匀不变、Al组分均匀不变这4种不同结构反射式光电阴极的分辨力特性.分析了Al组分、掺杂浓度、AlxGa1–x As层厚度、GaAs层厚度和入射光波长对阴极分辨力的影响.仿真结果表明,阴极材料中掺杂浓度梯度变化以及Al组分梯度变化都可以提高反射式AlxGa1–x As/GaAs光电阴极的分辨力,其中掺杂浓度线性变化的同时, Al组分线性变化对AlxGa1–x As/GaAs光电阴极分辨力的影响最为明显.仿真结果还表明:Al组分从0.45线性变化至0时,阴极分辨力最好;掺杂浓度从1019—1018 cm–3线性变化比保持1019 cm–3不变,阴极分辨力更好;而阴极中Al 相似文献
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通过建立和求解指数掺杂阴极中电子所遵循的二维连续性方程,得到了透射式指数掺杂阴极的调制传递函数表达式,并利用该表达式对阴极分辨力特性进行了理论计算和分析.计算结果显示,与均匀掺杂相比,指数掺杂能较明显地提高阴极的分辨力.当空间频率f在100—400 lp/mm范围时,分辨力的提高最为明显,如当f=200 lp/mm时,分辨力一般可提高20%—50%.与量子效率的提高相同,指数掺杂阴极分辨力的提高也是内建电场作用的结果.
关键词:
指数掺杂
内建电场
分辨力
调制传递函数 相似文献
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通过在一维连续性方程光电子产生函数项中加入短波约束因子,修正了指数掺杂和均匀掺杂透射式GaAs光电阴极量子效率公式.利用修正的透射式阴极量子效率公式分别拟合制备的指数掺杂和均匀掺杂透射式阴极量子效率实验曲线,符合得很好.另外拟合得到的阴极性能参数表明,由于内建电场的作用,指数掺杂阴极的性能要好于均匀掺杂阴极,指数掺杂结构能够明显提高透射式阴极的量子效率.
关键词:
透射式光电阴极
指数掺杂
量子效率
内建电场 相似文献
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将GaAs光电阴极发射层掺杂浓度由体内到发射表面从高到低的进行指数掺杂,能在发射层形成一个恒定的内建电场,有利于光电子的逸出.在考虑内建电场的作用下,通过建立和求解少数载流子所遵循的一维连续性方程,得到了反射式和透射式指数掺杂阴极的量子效率公式,并利用这些公式对其量子效率进行了理论计算和仿真.计算结果显示发射层指数掺杂能较明显的提高阴极的量子效率,与均匀掺杂阴极相比,能使反射式阴极积分灵敏度提高约20%,透射式阴极提高30%以上.指数掺杂提高阴极量子效率的主要原因与内建电场有关,光电子在内建电场作用下以扩散加漂移的方式到达阴极表面,从而减小了后界面复合速率对阴极的影响,同时提高了阴极的等效电子扩散长度.
关键词:
指数掺杂
内建电场
能带结构
量子效率 相似文献
5.
讨论了一种具有超快时间响应特性的新光电阴极, 即大梯度指数掺杂透射式GaAs 负电子亲和势 (NEA) 光电阴极, 模拟了它的量子效率、时间分辨和空间分辨能力等特性. 理论分析结果表明, 由于大梯度指数掺杂设计方式, 在吸收层内形成较大的内建电场, 因此光生电子在GaAsNEA阴极内的渡越时间大大缩短, 当GaAs吸收层厚度~0.9 μm时, 其响应时间达到~ 10 ps, 说明这种新NEA阴极具有远优于传统均匀掺杂NEA阴极的超快响应特性. 同时在整个光谱响应范围内, 量子效率达到约10%-20%, 空间分辨力显著高于以往的计算结果. 分析结果表明,在保证较高的量子效率条件下, 这种新阴极能够突破常规GaAsNEA阴极的时间分辨率极限, 提高GaAsNEA阴极本身的分辨力, 有望用于超快摄影、电子加速器和自由电子激光器的电子源等领域, 进一步扩展NEA光电阴极的应用范围. 相似文献
6.
双近贴聚焦微光像增强器分辨力理论极限问题研究 总被引:1,自引:1,他引:0
分辨力和MTF是微光像增强器的2个重要参数。根据线性系统傅里叶频谱理论,分析了微光像增强器的MTF和分辨力特性。 计算出理想条件下,基于光阴极/MCP/荧光屏3部件结构以及带内电子增益机制的光阴极/荧光屏2部件结构的近贴聚焦像管的理论极限分辨力。它们分别是96.6lp/mm和98.1lp/mm。该结果可供人们改进像管MTF及分辨力特性时参考。 相似文献
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《物理学报》2017,(6)
从变掺杂负电子亲和势(NEA)Ga N光电阴极材料的光电发射机理入手,给出了反射式变掺杂NEA Ga N光电阴极内建电场和量子效率的计算公式.利用初步设计的变掺杂NEA Ga N光电阴极,介绍了变掺杂NEA Ga N阴极的激活过程和激活光电流的变化特点.结合国内外典型的变掺杂NEA Ga N阴极的量子效率曲线,分析了Ga N光电阴极量子效率曲线的特点.结果显示:由于内建电场的存在,反射式变掺杂NEA Ga N光电阴极量子效率在240 nm处即可达到56%,在较宽的入射光波长范围内,阴极具有相对平稳的量子效率,量子效率值随入射光子能量的增加而增加,并且量子效率曲线在阈值附近表现出了明显的锐截止特性. 相似文献
9.
本文提出了一种可提高透射式GaAs光电阴极响应速度的阴极结构方案,并对这种结构的透射式GaAs光电阴极在电场作用下的响应时间进行了理论计算。计算结果表明,这种结构可便透射式GaAs光电阴极的响应时间由1ns左右减少到几个或几十个ps。 相似文献
10.
用常压MOCVD装置,制备了透射式GaAs光电阴极材料。发射层P-型GaAs掺杂浓度到1018-1019cm-3,少子扩散长度到4.02μm。AlGaAs层的Al组分含量到0.83,其吸收光谱长波限与设计值基本符合。利用此材料进行了阴极激活实验,制成了透射式GaAs光阴极。 相似文献
11.
In order to research the transport characteristic of photoelectrons in different-structure transmission-mode GaAs photocathodes, the energy and emergence angle spreads of photoelectrons reaching the band-bending region are calculated and the photoemission properties are analyzed. Based on the established atomic configuration models and ionized impurity scattering formulas of the uniform-doping and exponential-doping photocathodes, the trajectories of photoelectrons in different GaAs photocathodes have been calculated. The results show that, the emergence angle spread of the exponential-doping photocathode is more centralized than that of the uniform-doping one. The influence of the built-in electric field on the photoemission is obvious in the short-wave region. The built-in electric field not only increases the quantum efficient, but also improves the resolution of photocathode. This research can be propitious to investigate the photoemission mechanism, and to analyze the effect of the excited photoelectrons on the image intensifier performance. 相似文献
12.
设计了具有e指数内建电场的透射式GaAs负电子亲和势阴极,利用数值计算方法研究了它的时间响应特性和量子效率特性。结果表明,当吸收区厚度L~0.2~1.5 μm时,阴极的响应时间和量子效率均随L的增大而增大;尤其当L~1.1 μm时响应时间达到10 ps,量子效率达到12.5%~20%,迄今为止,与其他GaAs光电阴极相比,在相同光谱响应条件下,该响应速度是最高的。另外,在不同L下,获得了平均时间衰减常数τ'的函数分布和能够获得最短响应时间的最优系数因子β分布,为新型高速响应GaAs光电阴极的时间响应和量子效率优化提供了必要的理论基础和数据支持。 相似文献
13.
In order to well study the internal body performance for transmission-mode GaAs photocathode of different varied doping structures, two GaAs photocathodes of exponential doping structure and gradient doping structure were designed respectively. Because surface photovoltage spectrum has close relation with the internal properties of GaAs photocathodes, the connection between surface photovoltage and internal electronic field was well discussed through deduction and calculation. The difference of two structures and the value of internal electronic energy were exactly calculated and verified by experiments. The internal band bending energy could form an internal electronic field with the same direction, which could help the photo-excited electrons to move toward surface barrier layer. This research shows a better method to well study the varied doping structures for GaAs photocathode materials and will help to improve the growth structure for transmission-mode GaAs photocathode module in the future. 相似文献
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Comparative research on the transmission-mode GaAs photocathodes of exponential-doping structures
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Early research has shown that the varied doping structures of the active layer of GaAs photocathodes have been proven to have a higher quantum efficiency than uniform doping structures. On the basis of our early research on the surface photovoltage of GaAs photocathodes, and comparative research before and after activation of reflection-mode GaAs photocathodes, we further the comparative research on transmission-mode GaAs photocathodes. An exponential doping structure is the typical varied doping structure that can form a uniform electric field in the active layer. By solving the one-dimensional diffusion equation for no equilibrium minority carriers of transmission-mode GaAs photocathodes of the exponential doping structure, we can obtain the equations for the surface photovoltage (SPV) curve before activation and the spectral response curve (SRC) after activation. Through experiments and fitting calculations for the designed material, the body-material parameters can be well fitted by the SPV before activation, and proven by the fitting calculation for SRC after activation. Through the comparative research before and after activation, the average surface escape probability (SEP) can also be well fitted. This comparative research method can measure the body parameters and the value of SEP for the transmission-mode GaAs photocathode more exactly than the early method, which only measures the body parameters by SRC after activation. It can also help us to deeply study and exactly measure the parameters of the varied doping structures for transmission-mode GaAs photocathodes, and optimize the Cs-O activation technique in the future. 相似文献
16.
Comparative research on the transmission-mode GaAs photocathodes of exponential-doping structures
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Early research has shown that the varied doping structures of the active layer of GaAs photocathodes have been proven to have a higher quantum efficiency than uniform doping structures.On the basis of our early research on the surface photovoltage of GaAs photocathodes,and comparative research before and after activation of reflection-mode GaAs photocathodes,we further the comparative research on transmission-mode GaAs photocathodes.An exponential doping structure is the typical varied doping structure that can form a uniform electric field in the active layer.By solving the one-dimensional diffusion equation for no equilibrium minority carriers of transmission-mode GaAs photocathodes of the exponential doping structure,we can obtain the equations for the surface photovoltage(SPV) curve before activation and the spectral response curve(SRC) after activation.Through experiments and fitting calculations for the designed material,the body-material parameters can be well fitted by the SPV before activation,and proven by the fitting calculation for SRC after activation.Through the comparative research before and after activation,the average surface escape probability(SEP) can also be well fitted.This comparative research method can measure the body parameters and the value of SEP for the transmission-mode GaAs photocathode more exactly than the early method,which only measures the body parameters by SRC after activation.It can also help us to deeply study and exactly measure the parameters of the varied doping structures for transmission-mode GaAs photocathodes,and optimize the Cs-O activation technique in the future. 相似文献