共查询到19条相似文献,搜索用时 125 毫秒
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《红外技术》2017,(12):1073-1077
针对GaN基光电阴极激活过程中Cs-O交替存在的光电流的增幅问题,本文主要比较了GaN和GaAs材料性质、表面结构以及激活过程中光电阴极的光电流。发现GaN的熔点高于GaAs,在制备GaN基光电阴极时则需要更高的热清洗温度;如果用双偶极子模型描述GaN(1000)和GaAs(100)表面的光电发射机理,GaN(1000)表面Cs原子与O原子形成第二偶极矩O-Cs,几乎"平躺"在表面,对光电发射贡献不大;GaAs(100)表面Cs原子与O原子形成第二偶极矩O-Cs几乎"垂直"于表面,降低了表面功函数,对光电发射贡献很大;Cs-O激活过程中,对于GaAs光电阴极,Cs、O交替过程形成的光电流与单纯Cs激活时的光电流相比,有几倍甚至上百倍的增长;GaN只提高了20%左右。通过第一性原理计算,与现在的GaN基(1000)面相比,GaN基的(11 2 0)和(10 1 0)面是极具潜力的光电发射面;预计闪锌矿GaN基(100)面会取得更好的结果。 相似文献
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时间分辨特性是GaAs光电阴极应用于泵浦探测等领域的一种极为重要的性能参量。采用矩阵差分求解光电子扩散模型的方式计算了光电子连续性方程和出射光电子流密度方程,发现影响GaAs光电阴极时间分辨特性的因素包括GaAs/GaAlAs后界面复合速率、GaAs电子扩散系数和GaAs激活层厚度,之后较为系统地研究了这三种物理因素对GaAs光电阴极时间分辨特性的影响。研究结果表明,GaAs电子扩散系数和GaAs/GaAlAs后界面复合速率与光电阴极的响应速率存在非线性正比关系,且随着两者的增大,GaAs光电阴极将出现饱和响应速率。激活层厚度对GaAs光电阴极响应时间的影响最大,通过激活层厚度的适当减薄可以将GaAs光电阴极的响应时间缩短至20 ps,可满足绝大多数光子、粒子探测的快响应需求。该研究为快响应GaAs光电阴极的实验和应用提供了必要的理论支撑。 相似文献
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为了提高Cs-O激活后GaAs光阴极的稳定性,延长像管的使用寿命,从Cs-O激活方面着手进行研究,寻找解决途径。改变GaAs光阴极激活中的Cs过量,并在线监测真空环境下光电流的变化情况,寻找激活对GaAs光阴极稳定性的影响因素。分别进行3组5种比例的激活实验,在光电流下降至Cs峰峰值90%、70%、50%、30%和10%时给O进行交替激活。激活结束后,在低于110-8Pa的真空环境下在线监控30min内的光电流,发现过Cs90%、70%、50%激活的光阴极稳定性好,过Cs30%次之,过Cs10%相对最差。结果表明:GaAs光阴极Cs-O激活时,Cs量越多,表面势垒的建构越完整,光阴极的稳定性就越好,对改善GaAs光阴极稳定性,延长使用寿命具有重要意义。 相似文献
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单色的 Hellα(hv=40.8eV)光电子发射测量发现:在IBA的 GaP(III)-1×1表面上,最外层Ga原子的3d能级结合能比体内减小0.75±0.05eV.解释为表面原子的极化程度低于体内. 相似文献
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单色的 Hellα(hv=40.8eV)光电子发射测量发现:在IBA的 GaP(III)-1×1表面上,最外层Ga原子的3d能级结合能比体内减小0.75±0.05eV.解释为表面原子的极化程度低于体内. 相似文献
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利用自行研制的光电阴极激活评估实验系统,对激活后的反射式GaN及GaAs光电阴极进行了稳定性测试,获得了Cs/O激活一段时间后阴极随时间变化的光谱响应,通过计算得到量子效率曲线.结果表明:激活结束后GaN灵敏度可以在较长时间内保持稳定,而后缓慢衰减.而GaAs光电阴极的光电流随时间近似呈指数衰减.结合阴极表面双偶极层结构以及表面化学成分,分析原因主要是:两种阴极表面进行Cs/O激活后形成的双偶极子的结构不同、衰减过程中双偶极层化学成分变化方式不同决定.GaN光电阴极激活后cs以复杂氧化物存在,更加稳定,灵敏度的衰减主要是由未分解的氧引起,而GaAs灵敏度下降的原因主要是表面双偶极层中的Cs极易脱附,影响其稳定性. 相似文献
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《Proceedings of the IEEE. Institute of Electrical and Electronics Engineers》1974,62(10):1339-1360
Semiconductors with negative electron affinity (NEA) surfaces are used as photoemitters, secondary emitters, and cold-cathode emitters. A comprehensive review of the characteristics and applications of these materials is presented, the concept of NEA is described, and a comparison is made between NEA and conventional emitters. Electron generation, transport, and emission processes of NEA emitters are discussed. NEA III-V compound photocathodes, especially GaAs, are described with respect to their fabrication, performance, and applications to photomultipliers and image intensifier tubes. The structure and performance of NEA secondary emitters are presented. NEA GaP secondary-emission dynodes represent the most important device application. NEA cold cathodes, using GaAs, Ga(As, P), or Si, have been investigated, and their performance characteristics are summarized. NEA Si cold cathodes have been incorporated in developmental TV camera tubes. The characteristics of these tubes are reviewed. 相似文献
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We have observed electron emission into vacuum from the exposed areas of a patterned p++-GaAs substrate which was coated with cesium and oxygen. The emission barrier is a double layer of titanium-tungsten/silicon nitride. The exposed areas of the cathode were activated to the negative electron affinity (NEA) condition. It has been an open question whether it would be possible to activate the exposed areas of a patterned GaAs cathode. This result opens the possibility of utilizing NEA cathode technology for projection electron beam lithography tools, NEA-based vacuum microelectronics devices, and a combination of bulk devices with NEA emitters. A picture of an emission pattern projected onto a phosphor screen is presented. Auger depth profile was used to determine the stability of the TiW/GaAs interface through the activation procedure. Short and long term current stability were measured. A technique for cathode recovery and reactivation has been developed 相似文献
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D. Sun D.W. Treat 《Photonics Technology Letters, IEEE》1996,8(1):13-15
We report the demonstration of TM polarized laser emission at 833 nm from GaAsP-AlGaAs quantum well laser structures grown on GaAs substrates by low-pressure organometallic vapor phase epitaxy for the first time. This is the longest wavelength near infrared TM polarized laser ever reported. Broad area laser diodes containing single GaAs/sub 0.95/P/sub 0.05/ quantum well lased at a low threshold current density of 280 A/cm/sup 2/ for a cavity length of 1 mm and with a high differential quantum efficiency of 32%/facet for cavity length less than 500 /spl mu/m. 相似文献
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《Microelectronics Journal》2004,35(1):7-11
In segregation during InAs growth on GaAs(001) is studied using a real time, in situ technique capable of measuring sample accumulated stress. A 50% surface In segregation of liquid-like stress free matter is deduced. A picture of growth below critical thickness for quantum dot formation is discussed on the basis of the equilibrium between pseudomorphic InAs and liquid In dominated by the stress energy. Quantum rings are produced when large (>10 nm height) quantum dots are covered with 2 nm of GaAs cap. A formation mechanism of the rings is presented. The possibility of tailoring photoluminescence emission through control over size and shape is demonstrated. 相似文献
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A GaAs/GaAlAs transmission photocathode surface topography is examined with a scanning electron microscope(SEM)in the secondary emission mode.The contributions of photocathode surface topography to mean transverse energy of electrons emitted from the photocathode are calculated.Measurement is made of the variation of mean transverse emission energy with activating time during the course of activation.It is shown that the scattering of the photoelectrons in the Cs/O layer is the primary cause of the unexpectant high values of the mean transverse energy of electrons emitted from GaAs/GaAlAs photocathod.A method is proposed for the reduction of te mean transverse energy of electrons emitted from the photocathode. 相似文献
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用扫描电镜观测了 Ga As/ Ga Al As 透射式光电阴极的表面形貌,计算了阴极表面形貌对阴极发射电子的平均横向能量的贡献,测量了阴极激活过程中阴极发射电子的平均横向能量随激活时间的变化。结果表明, Ga As/ Ga Al As 阴极表层的 Cs/ O 激活层对电子的散射是导致阴极发射电子的平均横向能量值增高的根本原因。最后提出减少阴极发射电子的平均横向能量的技术途径。 相似文献
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The Raman spectra of a porous doped GaAs(100) crystal were studied. It is established that emission in the plasma-phonon spectra of both the starting and porous crystals is highly polarized and is independent of the incident-radiation polarization. It is inferred that the contribution of the Froelich mechanism to the intensity of the plasma-phonon spectrum is predominant and that the effects of defects and multiple scattering on the scattered-light polarization in porous GaAs may be ignored. The cause for the violation of the selection rules in the spectrum of porous crystal is discussed. 相似文献
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A novel vacuum microelectronic electron emitter has been demonstrated in GaAs by using a planar-doped-barrier (PDB) structure. Emitted electrons are collected in high vacuum by a tantalum anode placed ~1 mm away from the emitter surface. Surface passivation with (NH 4)2Sx followed by in situ heating in vacuum has been used to obtain an atomically clean surface. An emission current density of 0.42 A-cm-2 and an efficiency of 0.3% have been obtained from a 60 μm×60 μm emission region with an anode bias of 100 V 相似文献