原子核物理评论
原子覈物理評論
원자핵물리평론
Nuclear Physics Review
2014年
1期
81-85
,共5页
习凯%刘杰%张战刚%耿超%刘建德%古松%刘天奇%侯明东%孙友梅
習凱%劉傑%張戰剛%耿超%劉建德%古鬆%劉天奇%侯明東%孫友梅
습개%류걸%장전강%경초%류건덕%고송%류천기%후명동%손우매
单粒子效应%δ电子分布%多位翻转%Geant4
單粒子效應%δ電子分佈%多位翻轉%Geant4
단입자효응%δ전자분포%다위번전%Geant4
single event effect%radial ionization profile%multiple bit upset%Geant4
随着微电子器件集成度增加,由入射离子在器件灵敏区内引起的δ电子分布对器件单粒子效应的影响越来越显著;尤其是它极易引发多位翻转,严重影响设计加固的有效性。首先利用蒙特卡罗软件包Geant4模拟得到重离子在器件灵敏区内产生的δ电子分布,分析得出以下规律:入射离子单核能越高,其产生δ电子分布的径向范围越大;单核能相同的不同种离子,原子序数越大其产生的δ电子密度越大。其次,通过模拟一款45 nm 静态随机存储器的单粒子翻转效应,说明δ电子和灵敏区分布共同影响器件的多位翻转。当器件灵敏区间距一定时,多位翻转率随入射离子能量的升高先上升后下降;在多位翻转率峰值和布喇格峰之间,多位翻转率随入射离子线性能量传输(LET)值的升高而降低,在该区域两侧多位翻转率随离子LET值的升高而升高。
隨著微電子器件集成度增加,由入射離子在器件靈敏區內引起的δ電子分佈對器件單粒子效應的影響越來越顯著;尤其是它極易引髮多位翻轉,嚴重影響設計加固的有效性。首先利用矇特卡囉軟件包Geant4模擬得到重離子在器件靈敏區內產生的δ電子分佈,分析得齣以下規律:入射離子單覈能越高,其產生δ電子分佈的徑嚮範圍越大;單覈能相同的不同種離子,原子序數越大其產生的δ電子密度越大。其次,通過模擬一款45 nm 靜態隨機存儲器的單粒子翻轉效應,說明δ電子和靈敏區分佈共同影響器件的多位翻轉。噹器件靈敏區間距一定時,多位翻轉率隨入射離子能量的升高先上升後下降;在多位翻轉率峰值和佈喇格峰之間,多位翻轉率隨入射離子線性能量傳輸(LET)值的升高而降低,在該區域兩側多位翻轉率隨離子LET值的升高而升高。
수착미전자기건집성도증가,유입사리자재기건령민구내인기적δ전자분포대기건단입자효응적영향월래월현저;우기시타겁역인발다위번전,엄중영향설계가고적유효성。수선이용몽특잡라연건포Geant4모의득도중리자재기건령민구내산생적δ전자분포,분석득출이하규률:입사리자단핵능월고,기산생δ전자분포적경향범위월대;단핵능상동적불동충리자,원자서수월대기산생적δ전자밀도월대。기차,통과모의일관45 nm 정태수궤존저기적단입자번전효응,설명δ전자화령민구분포공동영향기건적다위번전。당기건령민구간거일정시,다위번전솔수입사리자능량적승고선상승후하강;재다위번전솔봉치화포나격봉지간,다위번전솔수입사리자선성능량전수(LET)치적승고이강저,재해구역량측다위번전솔수리자LET치적승고이승고。
As the size of the transistor sensitive volume is decreased with the technology generation, the radial distribution ofδ-electrons around the ion path has become more and more important to SEE(Single Event Effects) in semiconductor devices. Because it tends to, by causing MBU(Multiple-bit Upsets), invalidate error correcting codes which allow the device to work properly even when errors occur. In this work, Geant4 toolkit was used to simulate the radial ionization profile of heavy ions with different parameters. From the simulation, the certain rules were deduced: the higher the ion energy per nucleon, the wider the radial ionization track;for an identical energy per nucleon, the heavier the ion, the higher the electron density in track core. Then by simulating SEU(Single Event Upsets) of a 45 nm static random access memory (SRAM), effects of ion track structure on its MBU were illustrated. The maximum value of the MBU probability is determined not only by the structure of the device but also by the distribution of theδ-electrons generated by the incident ion. For ion energies between the top of the curve and the Bragg Peak, the MBU probability of the device decreases with the increasing LET values. For other ion energies, the probability increases as LET increasing.