共查询到17条相似文献,搜索用时 109 毫秒
1.
研究了低电压的人体模型(HBM)静电放电(ESD)对微电子器件造成的潜在失效。分别从CB结和EB结对2SC3356晶体管施加低电压HBM的ESD应力,结果表明:从CB结施加低电压的ESD电应力,所产生的潜在失效的几率要高于从EB结施加低电压的ESD电应力产生的潜在失效几率,即CB结比EB结对低电压的ESD应力引入的潜在失效更为敏感。高温(≥125 ℃)寿命实验有退火效应,从而缓解了低电压的ESD应力使器件产生的潜在损伤,使静电放电过程中引入的潜在损伤自恢复。 相似文献
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静放电电磁脉冲模拟装置 总被引:1,自引:0,他引:1
介绍了静电放电电磁脉冲(ESD EMP)的特性,研究了用ESD模拟器产生ESD EMP的方法,并给出了ESD EMP的时域波形和频谱。在研究ESD模拟器的基础上,首次通过ESD模拟器和GTEM室的结合,在GTEM室内产生了均匀的,重复性和线性好的ESD EMP。实验表明,用这种能够实验对静电放电电磁脉冲的实验室模拟,实验了人们用GTEM室产生ESD EMP的梦想。 相似文献
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系统级静电放电(ESD)效应仿真可以在电子系统进行测试之前进行有效的静电放电效应防护,缩短研发周期。根据传输线脉冲测试(TLP)结果,对瞬态电压抑制(TVS)二极管和芯片引脚进行spice行为建模,结合ESD脉冲源的等效电路模型,PCB板的S参数模型,采用场路协同技术完成了系统级静电放电效应的仿真。针对一个典型的电子系统,在IEC 61000-4-2 ESD应力作用下,完成了一款开关芯片防护电路的仿真,并对电路进行了加工、放电测试,仿真与测试芯片引脚的电压波形吻合良好,验证了该仿真方法的有效性。 相似文献
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基于Rompe-Weizel火花动态电阻公式,数值计算了电容器经火花开关放电时负载电阻上的输出电压。在相同电参数条件下,计算所得的峰值电压为54 kV,前沿为2.0 ns,与实验所得的55 kV和2.3 ns基本吻合。基于Braginskii火花动态电阻公式,在假定火花开关电导率恒定与电导率渐变的条件下,利用传输线放电电路数值计算了气体火花开关的非线性动态电阻。与已有实验测量结果(0.7~0.9 Ω)对比,发现电导率渐变模型(0.5~0.8 Ω)更适合用于反映火花开关的动态电阻变化过程。进而在此模型中引入了负载电阻项,通过计算负载端的透射电流,数值计算得单脉冲形成线对负载放电时的电压脉冲前沿为7~9 ns,而利用单线经高压氢气自击穿火花开关放电得到初步实验结果为8 ns。 相似文献
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采用基于半导体漂移扩散模型的数值模拟软件对高功率微波(HPM)作用下GGMOS型的静电放电(ESD)防护器件效应进行了数值模拟研究。对ESD器件在HPM作用下的响应特性及器件内部的物理图像进行了数值模拟。数值模拟的结果表明,外部注入HPM信号的幅值和频率是影响ESD器件的因素,在加载30ns脉宽的HPM脉冲作用下,器件内部达到的最高温度与信号幅值成正指数关系。在给ESD注入相同幅值的HPM信号时,频率越大,器件达到失效温度所需要的时间越长。 相似文献
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分析了静电放电(ESD)辐射场的偶极子模型。用高采样速率数字示波器和定做的宽带电磁与磁场探头测量了计算机操作中人体静电放电产生的瞬态电场与磁场。用FFT分析了静电放电辐射场的频谱。研究了静民放电辐射场对某电路高频信号的影响。研究结果表明,即使是很低电压(2kV)的静电放电,其辐射近场的电场达几百V/m,磁场可达几十A/m静电放电辐射场的频谱极宽,从数兆赫到数千兆赫。静电放电对高频电路的试验结果表明,若不采取有效的防护措施,人体静电放电辐射电磁场会对电路造成一定的影响,如对集成电路与元器件造成“潜在效应”的损害,对电路造成电磁干扰,甚至损坏电子器件。 相似文献
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基于对静电放电(electrostatic discharge,ESD)应力下高电压、大电流特性的研究,本文通过优化晶格自加热漂移-扩散模型和热力学模型,并应用优化模型建立了全新的0.6 μm CSMC 6S06DPDM-CT02 CMOS工艺下栅接地NMOS (gate grounded NMOS,ggNMOS)ESD保护电路3D模型,对所建模型中漏接触孔到栅距离(drain contact to gate spacing,DCGS)与源接触孔到栅距离(source contact to gate sp
关键词:
栅接地NMOS
静电放电
漏接触孔到栅的距离
源接触孔到栅的距离 相似文献
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针对飞行器全球卫星导航系统接收机易受静电放电干扰的问题,研究了机体表面电晕放电与机务维修火花放电对接收机的干扰效应。分析了静电放电的时频域特征,使用针球电极与高压源组成的模拟器开展了电晕放电对接收机的前门耦合实验,证明了电晕脉冲产生的辐射场对接收机无明显干扰效应。基于人体金属ESD模型开展了火花放电对接收机的干扰效应实验,发现浪涌电流易导致接收机串口转换芯片电位波动,读写程序主循环卡死,应针对串口端进行静电阻抗器防护。 相似文献
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典型静电放电火花点燃能力测试研究 总被引:1,自引:1,他引:0
通过对静电放电火花点火过程的物理特征研究,分析与总结了典型静电放电火花的点燃能力.根据放电火花的产生条件和形状特点,静电放电火花分为电晕放电、刷形放电、料仓堆表面放电、人体放电、火花放电和传播型尉形放电6种典型放电类型.根据静电放电火花的火花空间分布范围和火花持续时间,研究了静电放电火花点燃可燃物的能力.典型静电放电火花的实际点火能量为:电晕放电不大于0.025mJ,刷形放电不大于3mJ,料仓堆表面放电不大于10mJ.人体放电不大于30mJ,火花放电不大于1J,传播型刷形放电不大于10J. 相似文献
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《Journal of Electrostatics》2005,63(6-10):577-582
Electrostatic discharge (ESD) is an important source of accidental ignitions in process industries and damage to semiconductor electronic devices. There is a need to understand the time-varying ESD event and interaction between ESD probe and source in order to understand the important parameters in ESD measurements for evaluation of these phenomena.This paper compares measured peak current, waveform, risetime and charge transferred in ESD from charged isolated spherical conductors with and without a ground plane (spark), and triboelectrically charged polyethylene and polyamide samples (brush discharge). Measurements made using two recently developed ESD probes are compared. 相似文献
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静电放电电磁脉冲模拟装置 总被引:1,自引:0,他引:1
介绍了静电放电电磁脉冲(ESD EMP)的特性。研究了用ESD 模拟器产生ESD EMP的方法,并给出了ESD EMP的时域波形和频谱。在研究ESD模拟器的基础上,首次通过ESD模拟器和GTEM室的结合,在GTEM室内产生了均匀的、重复性和线性好的ESD EMP。实验表明,用这种装置能够实现对静电放电电磁脉冲的实验室模拟。实现了人们用GTEM室产生ESD EMP的梦想。 相似文献
16.
A curve-fitting method based on backpropagation (BP) neural network (NN) is proposed for fitting electrostatic discharge (ESD) current waveforms and giving the corresponding expressions in order to analyze the characteristics of ESD and calculate the ESD electromagnetic pulse radiation field. According to IEC61000-4-2, this method is used to fit the ideal contact current waveform of human-metal ESD to obtain the mathematical expression. The waveform parameters of the fitting curve meet the requirements of the IEC61000-4-2. By fitting the measured air ESD current waveform at 4 kV discharge, the mathematical expression is obtained. This paper proposes the mathematical expression for arbitrary curves and analyzes the factors affecting the effects of curve-fitting. 相似文献
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《Journal of Electrostatics》2007,65(2):75-81
We have investigated whether any force is generated by a spark discharge in a pin-to-plate system. Because it was difficult to measure the force directly over a short sparking period, three independent methods were employed to evaluate the magnitude of the force indirectly: (1) Axial vibration was observed for the pin electrode supported flexibly by a cantilever to the axial direction at the spark discharge that occurred periodically. The force was implicitly calculated in the case that the calculated vibration agreed with the measured. The result indicated that the force was almost 0 N during the spark period. The vibration was generated not by the force at the spark discharge but by alternative force of the Coulomb force at the period of no discharge and reaction force due to the ionic wind at the corona discharge. (2) A similar investigation was conducted whether the vibration magnitude depended on the spark current based on the assumption that the force at spark discharge depends on the spark current if any substantial force is generated at the spark discharge. We deduced that the force was not generated during the spark period and it was irrelevant to the spark current. (3) We made a hypothesis that axial vibration of the pin electrode could be observed if the spark discharge did not take place but the varying voltage was applied of which pattern was common with that with the spark discharge. To confirm the hypothesis an experiment was conducted with two parallel-connected pin-to-plate systems, the air gap of one system was slightly shorter than the other. The axial vibration was observed even in the system that the spark discharge did not take place and the vibration agreed also with the calculated. These three results suggested that no substantial force was generated at the spark period. 相似文献