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空间材料二次电子发射特性测试 总被引:9,自引:4,他引:5
空间材料的二次电子发射系数是表征航天器表面充电状态的重要参数 ,对于卫星表面带电的预测及卫星防带电设计选材具有重要的作用。为了测量空间材料二次电子发射特性 ,研制了专门的测试装置。介绍了该实验装置的主要结构、性能及技术指标等 ,通过应用计算机数据采集系统 ,并研制专门的数据处理软件 ,提高了装置的自动测量能力。实验说明 ,该装置用于空间材料的二次电子发射特性测试中测量方便、准确 相似文献
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航天器表面材料二次电子发射特性研究 总被引:2,自引:0,他引:2
《真空科学与技术学报》2021,(8)
航天器在轨表面入射离子、电子产生的二次发射电子流随二次电子发射系数的变化而变化,通过建模仿真对二次电子发射系数对充电电流、充电电位的影响进行验证。通过对航天器用表面材料ITO(Indium tin oxide,氧化铟锡)膜二次发射电子系数测试,测试结果与标准参数基本一致;测试结果表明,二次电子发射系数与材料厚度相关,且随着材料厚度的增加二次电子发射系数减小,因此可以通过改变航天器表面材料厚度的方式影响表面材料的二次电子发射系数,从而控制航天器表面材料的带电状态。 相似文献
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绝缘膜正带电现象在集成电路芯片低能电子束检测方面具有可以利用的前景。采用简化的表面电位分布模型 ,通过数值方法计算了二次电子从正带电绝缘膜表面发射后的运动轨迹 ,分析了初始条件和电位分布形态对轨迹特性的影响。在轨迹计算和考虑二次电子发射概率分布的基础上得到了二次电子受局部电场作用而返回表面时的最大初始动能、分布规律 ,提出了通过简单的一维势垒模型来确定二次电子返回率的方法 ,为分析电子束照射绝缘膜时正带电效应所产生的二次电子信号衬度现象奠定了基础 相似文献
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简述了热解石墨、高纯各向同性石墨和无氧铜材料的二次电子发射特性,以及离子束表面改性对二次电子发射特性的影响。分析表明热解石墨和高纯各向同性石墨的二次电子发射系数均明显低于无氧铜的二次电子发射系数,并且通过离子束表面改性后二次电子发射系数能够得到进一步的降低。同样的,离子束表面改性后的无氧铜的二次电子发射系数也得到一定的降低,并且还有很大的发展空间。 相似文献
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《真空科学与技术学报》2021,(1)
SMILE卫星在轨科学探测为大倾角椭圆轨道,在轨将遭遇多种等离子体环境,卫星表面带电状态将影响卫星在轨安全性和科学探测任务。在有限元建模的基础上,利用SPIS(Spacecraft Plasma Interaction System)软件仿真和评估了SMILE卫星在轨表面带电特性。仿真结果显示,卫星在不同环境下的表面充电电位存在差异,但不会影响科学载荷的数据获取。通过分析各种等离子体环境下充电电流,发现二次电子发射电流和光照区光电流对卫星表面充电起主导作用。卫星表面ITO膜阻值对卫星电位产生影响。 相似文献
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氧化镁因其二次电子发射系数高、抗溅射能力强等优异的性能,广泛应用于平板显示器等电子器件中,其二次电子发射性能有重要的研究价值。介绍了离子轰击下氧化镁薄膜发射的二次电子的典型测量装置及相关研究结论,总结了离子轰击下氧化镁薄膜二次电子的发射特性,同时对离子轰击的材料产生的二次电子发射的研究提出了建议。脉冲中和法比较适用于离子轰击下的氧化镁薄膜的二次电子发射的测量;不同晶面的MgO薄膜的二次电子发射系数不同,(111)晶面最高;低能离子入射情况下,二次电子的能量分布与离子类型无关。 相似文献
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Lee EJ Jung CH Hwang IT Choi JH Cho SO Nho YC 《ACS applied materials & interfaces》2011,3(8):2988-2993
A simple and controllable one-step method to fabricate superhydrophobic surfaces on poly(tetrafluoroethylene) (PTFE) films is developed on the base of electron irradiation. When the thickness of PTFE films is higher than the penetration depth of electron beams, electrical charging occurs at the surface of the films because of the imbalance between the accumulation of incident electrons and the emission of secondary electrons. Local inhomogeneity of charge distribution due to this electrical charging results in the nonuniform decomposition of PTFE molecular bonds. As electron fluence increases, surface morphology and surface roughness of the films are dramatically changed. An extremely rough surface with micrometer-sized pores is produced on the surface of PTFE films by electron irradiation at a fluence higher than 2.5 × 10(17) cm(-2).Because of high surface roughness, the irradiated PTFE films exhibit superhydrophobic property with a water contact angle (CA) greater than 150° at fluences ranging from 4 × 10(17) to 1 × 10(18) cm(-2). The surface morphology and corresponding water CA can be controlled by simply changing the electron fluence. This electron irradiation method can be applicable to the fabrication of superhydrophobic surfaces using other low-surface-energy materials including various fluoropolymers. 相似文献
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We report a detailed study of the electron emission from MgO and Y2O3 induced by the impact of 0.1-1 keV Ar+ ions. The mechanisms of ion-induced secondary electron emission from oxides are far less understood because charging of the target surface during ion irradiation prohibits the precise measurement of electron yield. For this study, targets were prepared by depositing 20 nm thick films of MgO and Y2O3 on the semi-conducting SnO2 substrate, which helps in charge neutralization. Additionally, a pulsed ion beam was used to further reduce the surface charging. It was found that the electron yield of both targets increases with energy of the ion. However, at a given ion energy the electron yield of Y2O3 was larger than MgO. Another important result of this study is that the electron emission from these large band gap insulators did not show any threshold effect, in contrast to the metal targets. It may be due to local reduction of the band gap through electron promotion processes. In addition, a Monte Carlo program was used to calculate the yield of secondary electrons excited by projectile ions, recoiling target atoms and electron cascades, and average escape depth of the secondary electrons emitted from the MgO and Y2O3 thin films. 相似文献
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Using a sol-gel precursor, Na-ion-doped MgO was prepared and applied to alternative current plasma display panels (ac-PDP). The cathodoluminescence spectra showed that the F+ center was increased as the concentration of Na+ was increased. Numerous pores were found on the printed MgO surface and seemed to give higher memory margin of ac-PDP compared to an electron beam-evaporated MgO film. All doped MgO showed higher secondary electron emission than printed pure MgO, likely owing to the O defect states of MgO. In addition, this result indicated the operational memory margin of the ac-PDP was directly proportional to the grade of surface charging. 相似文献