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Analysis of Charging Kinetics of Oxide Ceramics under Short Electron Beam Irradiation: Numerical Simulation of Secondary Electron Emission

机译:短电子束照射下氧化物陶瓷充电动力学的分析:二次电子发射的数值模拟

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This analysis is connected with the evolution of trapped charges, during electron injection, using a defocused electron beam of a Scanning Electron Microscope especially equipped with a secondary electron low-noise detector. Hence, during pulses of about ten ms, giving injection doses of a few pC, the measurements of the influence induced currents, Iind(t), due to the image charges Qind (t) in the metallic holder (corresponding to the trapped charges Qp (t) in the sample) and the total secondary electron currents, I??(t), can be carried out. Considering the experimental conditions defined by small primary current density (#104 pA/cm2) and low surface charge density (#10 pC/cm2), the relation, I0 = Iind(t) + I?? (t) can be verified [1] leading to (after integration over the injection time) a charge balance: Qinj = Qind+Q?? = Qp+Q?? The secondary electron emission yield, see(t) = 1 -^s{ Iind (t) / [Iind (t)+I?? (t)] }, is experimentally studied as a function of Qp(t). A simulation, which corresponds to a new mathematical model describing the spatial and temporal charge trapping, computes the temporal evolution of the secondary electron emission, see(t), as a function of net trapped charge, Qp(t), for various values of the kinetic energy of the primary electrons. The comparison between experimental results and numerical simulations would permit to evaluate absorption and transfer cross sections as well as mobility of the secondary electrons.
机译:在电子注入期间,使用扫描电子显微镜的离焦电子束,该分析与截止的电子束具有尤其配备有二次电子低噪声检测器。因此,在大约十毫秒的脉冲期间,注射少量PC的注射剂量,由于图像电荷Q IND IND (T)的测量值。金属支架中的INF>(t)(对应于捕获的电荷Q P (t)中的)和样品中的总电流,I ?? (t ),可以进行。考虑到由小初级电流密度定义的实验条件(#10 4 PA / cm 2 )和低表面电荷密度(#10 pc / cm 2 ),关系,i 0 (t)+ i ?? (t)可以验证[1]领先到(在注射时间上集成后)充电平衡:Q Inj = Q IND + Q ?? = Q P < / inf> + q ?? 次要电子发射产量,见(t)= 1 - ^ s {i ind (t)/ [i ind < / INF>(t)+ I ?? (t)]},作为Q P (t)的功能进行了实验研究。对应于描述空间和时间电荷捕获的新数学模型的模拟计算二次电子发射的时间演变,参见(t),作为净捕获的电荷,q p (t),用于主要电子的动能的各种值。实验结果与数值模拟之间的比较将允许评估吸收和转移横截面以及二次电子的迁移率。

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