首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 15 毫秒
1.
王晓晗  郭红霞  雷志锋  郭刚  张科营  高丽娟  张战刚 《物理学报》2014,63(19):196102-196102
文章提出了一种基于蒙特卡洛和器件仿真的存储器单粒子翻转截面获取方法,可以准确计算存储器单粒子效应,并定位单粒子翻转的灵敏区域.基于该方法,计算了国产静态存储器和现场可编程门阵列(FPGA)存储区的单粒子效应的截面数据,仿真结果和重离子单粒子效应试验结果符合较好.仿真计算揭示了器件单粒子翻转敏感程度与器件n,p截止管区域面积相关的物理机理,并获得了不同线性能量转移(LET)值下单粒子翻转灵敏区域分布.采用蒙特卡洛方法计算了具有相同LET、不同能量的离子径迹分布,结果显示高能离子的电离径迹半径远大于低能离子,而低能离子径迹中心的能量密度却要高约两到三个数量级.随着器件特征尺寸的减小,这种差别的影响将会越来越明显,阈值LET和饱和截面将不能完全描述器件单粒子效应结果.  相似文献   

2.
张战刚  雷志锋  岳龙  刘远  何玉娟  彭超  师谦  黄云  恩云飞 《物理学报》2017,66(24):246102-246102
基于蒙特卡罗方法研究空间高能离子在65—32 nm绝缘体上硅静态随机存取存储器(SOI SRAM)中产生的灵敏区沉积能量谱、单粒子翻转截面和空间错误率特性及内在的物理机理.结果表明:单核能为200 MeV/n的空间离子在60—40 nm厚的灵敏区中产生的能损歧离导致纳米级SOI SRAM在亚线性能量转移阈值区域出现单粒子翻转;宽的二次电子分布导致灵敏区仅能部分收集单个高能离子径迹中的电子-空穴对,致使灵敏区最大和平均沉积能量各下降25%和33.3%,进而引起单粒子翻转概率降低,以及在轨错误率下降约80%.发现俘获带质子直接电离作用导致65 nm SOI SRAM的在轨错误率增大一到两个数量级.  相似文献   

3.
使用中国散裂中子源提供的宽能谱中子束流,开展14 nm FinFET工艺和65 nm平面工艺静态随机存取存储器中子单粒子翻转对比研究,发现相比于65 nm器件,14 nm FinFET器件的大气中子单粒子翻转截面下降至约1/40,而多位翻转比例从2.2%增大至7.6%,源于14 nm FinFET器件灵敏区尺寸(80 nm×30 nm×45 nm)、间距和临界电荷(0.05 fC)的减小.不同于65 nm器件对热中子免疫的现象,14 nm FinFET器件中M0附近10B元素的使用导致其表现出一定的热中子敏感性.进一步的中子输运仿真结果表明,高能中子在器件灵敏区中产生的大量的射程长、LET值大的高Z二次粒子是多位翻转的产生诱因,而单粒子翻转主要来自于p,He,Si等轻离子的贡献.  相似文献   

4.
 报导了利用北京大学串列静电加速器提供的重离子对两类静态随机存储器进行单粒子效应的实验和测量。给出了两类静态随机存储器的单粒子效应翻转截面随线性能量转移值的变化关系曲线。  相似文献   

5.
 根据光的吸收机理,分析了单粒子效应脉冲激光模拟实验中所需用的脉冲激光的特点,探讨了脉冲激光单粒子效应的Monte Carlo计算模拟途径。在只考虑光电效应的简化下,得到存储器硅片单粒子翻转时入射脉冲激光能量阈值与临界电荷的计算关系式,进而给出该硅片的翻转截面的计算公式。在给定了存储器硅片的临界电荷的情况下,对入射脉冲激光能量阈值和单粒子翻转截面进行了计算。  相似文献   

6.
Dong-Qing Li 《中国物理 B》2022,31(5):56106-056106
Three-dimensional (3D) TCAD simulations demonstrate that reducing the distance between the well boundary and N-channel metal-oxide semiconductor (NMOS) transistor or P-channel metal-oxide semiconductor (PMOS) transistor can mitigate the cross section of single event upset (SEU) in 14-nm complementary metal-oxide semiconductor (CMOS) bulk FinFET technology. The competition of charge collection between well boundary and sensitive nodes, the enhanced restoring currents and the change of bipolar effect are responsible for the decrease of SEU cross section. Unlike dual-interlock cell (DICE) design, this approach is more effective under heavy ion irradiation of higher LET, in the presence of enough taps to ensure the rapid recovery of well potential. Besides, the feasibility of this method and its effectiveness with feature size scaling down are discussed.  相似文献   

7.
针对0.13 μm CMOS(Complementary Metal-Oxide-Semiconductor)体硅外延工艺下FPGA(Field Programmable Gate Arrays)配置片反熔丝PROM(Programmable-Read-Only-Memory)进行了单粒子效应(Single Event Effects SEEs)的加速器地面模拟试验研究。以PROM的存储容量、数据类型和工艺差异性为研究变量,考核与验证其在不同种类和能量粒子入射的系列性加速器地面SEEs模拟试验。研究结果表明,相对于8 Mbits PROM而言,空片16 Mbits PROM抗辐射性能最优,且从翻转饱和截面上说,16 Mbits的PROM具备更高的可靠性,优于国外同系列的芯片类型,试验用PROM芯片的单粒子锁定阈值>99.0 MeV·cm2/mg。另一方面,研究0.13 μm CMOS普通与深阱工艺技术下PROM芯片单粒子翻转效应异同性的实验数据表明,在高LET(Linear Energy Transfer)处的两者抗辐射性能并无明显变化,但是低LET处(LET翻转阈值)的加固效果较为明显,即抗辐射技术能力主要体现在LET翻转阈值的提升而非翻转截面的减小。Single event effects (SEEs) have been characterized and investigated on one-time configured devices for field-programmable-gate-arrays (FPGA) of programmable-read-only-memory (PROM) in 0.13 μm Complementary Metal-Oxide-Semiconductor (CMOS) technology.The variables of their memory size,written data and technology have been taken into consideration as the key parameters affecting the SEEs sensitivity when testing and verifying the reliability/radiation tolerance on self-made PROMs by heavy ions.The results show that,16 Mbits PROM within blanked data has been studied that it has better performance to radiation tolerance as compared with the 8 Mbits PROMs.Additionally,16 Mbits PROMs have the higher reliability,if based on the viewpoint of the saturated single event upset cross-section.To the single event latchup,16 Mbits PROMs were exposed to a total fluence of 107 ions/cm2 at the linear energy transfer (LET) of 99.0 MeV·cm2/mg and no obvious fluctuation of current has been observed.Additionally,as comparing the zone of high LET value,0.13 μm CMOS transistors with deep-well technology present a better radiation hardened approach than normal technology,especially in improving the threshold of LET at the zone of low LET value.  相似文献   

8.
Using a Monte Carlo simulation tool of the multi-functional package for SEEs Analysis(MUFPSA), we study the temporal characteristics of ion-velocity susceptibility to the single event upset(SEU) effect, including the deposited energy,traversed time within the device, and profile of the current pulse. The results show that the averaged dposited energy decreases with the increase of the ion-velocity, and incident ions of209 Bi have a wider distribution of energy deposition than132 Xe at the same ion-velocity. Additionally, the traversed time presents an obvious decreasing trend with the increase of ion-velocity. Concurrently, ion-velocity certainly has an influence on the current pulse and then it presents a particular regularity. The detailed discussion is conducted to estimate the relevant linear energy transfer(LET) of incident ions and the SEU cross section of the testing device from experiment and simulation and to critically consider the metric of LET.  相似文献   

9.
通过重离子实验研究了14-nm FinFET工艺静态随机存取存储器(SRAM)的单粒子翻转(SEU)特性。通过使用Weibull函数拟合SEU截面获得该器件的线性能量转移(LET)阈值:0.1 MeV/(mg/cm2)。对多位翻转(MBU)贡献的统计结果表明,当LET等于40.3 MeV/(mg/cm2)时,MBU的占比超过95%。此外,FinFET SRAM的SEU截面呈现出与Fin相关的入射角度的各向异性。该研究对基于FinFET工艺的抗辐射CMOS集成电路(IC)的设计具有一定的指导作用。  相似文献   

10.
秦军瑞  陈书明  梁斌  刘必慰 《中国物理 B》2012,21(2):29401-029401
Using computer-aided design three-dimensional (3D) simulation technology, the recovery mechanism of single event upset and the effects of spacing and hit angle on the recovery are studied. It is found that the multi-node charge collection plays a key role in recovery and shielding the charge sharing by adding guard rings. It cannot exhibit the recovery effect. It is also indicated that the upset linear energy transfer (LET) threshold is kept constant while the recovery LET threshold increases as the spacing increases. Additionally, the effect of incident angle on recovery is analysed and it is shown that a larger angle can bring about a stronger charge sharing effect, thus strengthening the recovery ability.  相似文献   

11.
针对特征尺寸为1.5 μm的国产静态随机存储器(SRAM),构建了三维SRAM存储单元模型,并对重离子引起的SRAM单粒子翻转效应进行了数值模拟.计算并分析了单粒子引起的单粒子翻转和电荷收集的物理图像,得到了SRAM器件的单粒子翻转截面曲线.单粒子翻转的数值模拟结果与重离子微束、重离子宽束实验结果比较一致,表明所建立的三维器件模型可以用来研究SRAM器件的单粒子翻转效应. 关键词: 三维数值模拟 单粒子翻转 微束 宽束  相似文献   

12.
重离子实验结果表明,具有高线性能量转移(LET)或大角度入射的快重离子导致静态随机存储器(SRAM)中的多位翻转(MBU)比例增大,甚至超过单位翻转比例。单个离子径迹中的电荷可以沿着径向扩散数个微米,被临近的灵敏区收集后引起MBU。器件灵敏区的各向异性空间布局与离子入射方向共同影响测试器件的MBU图形特征。位线接触点的纵向隔离导致横向型成为主要的两位翻转图形;"L"型和"田"型分别是主要的三位翻转和四位翻转图形。最后,对SRAM抗MBU加固设计和实验验证方法进行了讨论。  相似文献   

13.
We investigate the impact of heavy ion irradiation on a hypothetical static random access memory (SRAM) device. Influences of the irradiation angle, critical charge, drain-drain spacing, and dimension of device structure on the device sensitivity have been studied. These prediction and simulated results are interpreted with MUFPSA, a Monte Carlo code based on Geant4. The results show that the orientation of ion beams and device with different critical charge exert indispensable effects on multiple-bit upsets (MBUs), and that with the decrease in spacing distance between adjacent cells or the dimension of the cells, the device is more susceptible to single event effect, especially to MBUs at oblique incidence.  相似文献   

14.
电离总剂量(TID)与单粒子效应(SEE)是纳米SRAM器件在航天应用中的主要威胁。随着CMOS工艺的进步,两种辐射效应在纳米SRAM器件中的协同效应出现了一些新现象,有必要进一步开展深入研究。利用γ射线以及不同种类重离子对两款纳米SRAM器件开展了辐照实验,研究了不同辐照参数、测试模式以及数据图形条件下,电离总剂量对单粒子翻转(SEU)敏感性的影响。研究结果表明,γ射线辐照过后,存储单元中反相器开关阈值减小,漏电流增大,导致SRAM存储单元抗翻转能力降低,SEU截面有明显增大;未观察到"印记效应",数据图形对测试结果没有明显影响;多位翻转(MBU)比例无明显变化。  相似文献   

15.
针对90 nm和65 nm DDR(双倍数率)SRAM器件,开展与纳米尺度SRAM单粒子效应相关性的试验研究。分析了特征尺寸、测试图形、离子入射角度、工作电压等不同试验条件对单粒子翻转(SEU)的影响和效应规律,并对现有试验方法的可行性进行了分析。研究表明:特征尺寸减小导致翻转截面降低,测试图形和工作电压对器件单粒子翻转截面影响不大;随着入射角度增加,多位翻转的增加导致器件SEU截面有所增大;余弦倾角的试验方法对于纳米器件的适用性与离子种类和线性能量转移(LET)值相关,具有很大的局限性。  相似文献   

16.
The impact of ionizing radiation effect on single event upset(SEU) sensitivity of ferroelectric random access memory(FRAM) is studied in this work. The test specimens were firstly subjected to ~(60)Co γ-ray and then the SEU evaluation was conducted using ~(209)Bi ions. As a result of TID-induced fatigue-like and imprint-like phenomena of the ferroelectric material, the SEU cross sections of the post-irradiated devices shift substantially. Different trends of SEU cross section with elevated dose were also found, depending on whether the same or complementary test pattern was employed during the TID exposure and the SEU measurement.  相似文献   

17.
利用Monte Carlo方法,对14MeV中子引起存储器单粒子翻转过程进行了计算模拟,从而对引起单粒子翻转的关键因素——存储器灵敏区中的能量沉积进行了统计分析,为了解单粒子翻转随机过程提供了详细的能量沉积统计信息。The process of the single event upset induced by 14 MeV neutrons in SRAM silicon chip is simulated by using a Monte Carlo method. The deposited energies in sensitive volumes in the chip, which is an important factor in the single event upset, are statistically analysed. The statistic information about the deposited energies is provided for understanding the detailed random process of the single event upset.  相似文献   

18.
This paper presents a simulation study of the impact of energy straggle on a proton-induced single event upset(SEU)test in a commercial 65-nm static random access memory cell. The simulation results indicate that the SEU cross sections for low energy protons are significantly underestimated due to the use of degraders in the SEU test. In contrast, using degraders in a high energy proton test may cause the overestimation of the SEU cross sections. The results are confirmed by the experimental data and the impact of energy straggle on the SEU cross section needs to be taken into account when conducting a proton-induced SEU test in a nanodevice using degraders.  相似文献   

19.
The influence of the metric of linear energy transfer (LET) on single event upset (SEU), particularly multiple bit upset (MBU) in a hypothetical 90-nm static random access memory (SRAM) is explored. To explain the odd point of higher LET incident ion but induced lower cross section in the curve of SEU cross section, MBUs induced by incident ions 132Xe and 2~9Bi with the same LET but different energies at oblique incidence are investigated using multi-functional package for single event effect analysis (MUFPSA). In addition, a comprehensive analytical model of the radial track structure is incorporated into MUFPSA, which is a complementation for assessing and interpreting MBU susceptibility of SRAM. The results show that (i) with the increase of incident angle, MBU multiplicity and probability each present an increasing trend; (ii) due to the higher ion relative velocity and longer range of ~ electrons, higher energy ions trigger the MBU with less probability than lower energy ions.  相似文献   

20.
丁李利  郭红霞  陈伟  闫逸华  肖尧  范如玉 《物理学报》2013,62(18):188502-188502
基于解析分析对比了大尺寸与深亚微米尺度下静态随机存取存储器(static random access memory, SRAM)单元单粒子翻转敏感性的表征值及引入累积辐照后的变化趋势. 同时借助仿真模拟计算了0.18 μm工艺对应的六管SRAM单元在对应不同累积剂量情况下, 离子分别入射不同中心单管时的电学响应变化, 计算结果与解析分析所得推论相一致, 即只有当累积辐照阶段与单粒子作用阶段存储相反数值时, SRAM单元的单粒子翻转敏感性才会增强. 关键词: 累积辐照 单粒子翻转 静态随机存储器 器件仿真  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号