分享
ASTM_F_1192_-_11_2018.pdf
下载文档

ID:188572

大小:294.09KB

页数:11页

格式:PDF

时间:2023-03-04

收藏 分享赚钱
温馨提示:
1. 部分包含数学公式或PPT动画的文件,查看预览时可能会显示错乱或异常,文件下载后无此问题,请放心下载。
2. 本文档由用户上传,版权归属用户,汇文网负责整理代发布。如果您对本文档版权有争议请及时联系客服。
3. 下载前请仔细阅读文档内容,确认文档内容符合您的需求后进行下载,若出现内容与标题不符可向本站投诉处理。
4. 下载文档时可能由于网络波动等原因无法下载或下载错误,付费完成后未能成功下载的用户请联系客服处理。
网站客服:3074922707
TM_F_1192_ _11_2018
Designation:F119211(Reapproved 2018)Standard Guide for theMeasurement of Single Event Phenomena(SEP)Induced byHeavy Ion Irradiation of Semiconductor Devices1This standard is issued under the fixed designation F1192;the number immediately following the designation indicates the year oforiginal adoption or,in the case of revision,the year of last revision.A number in parentheses indicates the year of last reapproval.Asuperscript epsilon()indicates an editorial change since the last revision or reapproval.This standard has been approved for use by agencies of the U.S.Department of Defense.1.Scope1.1 This guide defines the requirements and procedures fortesting integrated circuits and other devices for the effects ofsingle event phenomena(SEP)induced by irradiation withheavy ions having an atomic number Z 2.This descriptionspecifically excludes the effects of neutrons,protons,and otherlighter particles that may induce SEP via another mechanism.SEP includes any manifestation of upset induced by a singleion strike,including soft errors(one or more simultaneousreversible bit flips),hard errors(irreversible bit flips),latchup(persistent high conducting state),transients induced in com-binatorial devices which may introduce a soft error in nearbycircuits,power field effect transistor(FET)burn-out and gaterupture.This test may be considered to be destructive becauseit often involves the removal of device lids prior to irradiation.Bit flips are usually associated with digital devices and latchupis usually confined to bulk complementary metal oxidesemiconductor,(CMOS)devices,but heavy ion induced SEPisalso observed in combinatorial logic programmable read onlymemory,(PROMs),and certain linear devices that may re-spond to a heavy ion induced charge transient.Power transis-tors may be tested by the procedure called out in Method 1080of MIL STD 750.1.2 The procedures described here can be used to simulateand predict SEP arising from the natural space environment,including galactic cosmic rays,planetary trapped ions,andsolar flares.The techniques do not,however,simulate heavyion beam effects proposed for military programs.The endproduct of the test is a plot of the SEP cross section(thenumber of upsets per unit fluence)as a function of ion LET(linear energy transfer or ionization deposited along the ionspath through the semiconductor).This data can be combinedwith the systems heavy ion environment to estimate a systemupset rate.1.3 Although protons can cause SEP,they are not includedin this guide.A separate guide addressing proton induced SEPis being considered.1.4 The values stated in SI units are to be regarded asstandard.No other units of measurement are included in thisstandard.1.5 This standard does not purport to address all of thesafety concerns,if any,associated with its use.It is theresponsibility of the user of this standard to establish appro-priate safety,health,and environmental practices and deter-mine the applicability of regulatory limitations prior to use.1.6 This international standard was developed in accor-dance with internationally recognized principles on standard-ization established in the Decision on Principles for theDevelopment of International Standards,Guides and Recom-mendations issued by the World Trade Organization TechnicalBarriers to Trade(TBT)Committee.2.Referenced Documents2.1 Military Standard:2750 Method 10803.Terminology3.1 Definitions of Terms Specific to This Standard:3.1.1 DUTdevice under test.3.1.2 fluencethe flux integrated over time,expressed asions/cm2.3.1.3 fluxthe number of ions/s passing through a one cm2area perpendicular to the beam(ions/cm2-s).3.1.4 LETthe linear energy transfer,also known as thestopping power dE/dx,is the amount of energy deposited perunit length along the path of the incident ion,typicallynormalized by the target density and expressed as MeV-cm2/mg.3.1.4.1 DiscussionLET values are obtained by dividingthe energy per unit track length by the density of the irradiatedmedium.Since the energy lost along the track generates1This guide is under the jurisdiction of ASTM Committee F01 on Electronicsand is the direct responsibility of Subcommittee F01.11 on Nuclear and SpaceRadiation Effects.Current edition approved March 1,2018.Published April 2018.Originallyapproved in 1988.Last previous edition approved in 2011 as F119211.DOI:10.1520/F1192-11R18.2Available from Standardization Documents Order Desk,Bldg.4,Section D,700 Robbins Ave.,Philadelphia,PA 191115094.Copyright ASTM International,100 Barr Harbor Drive,PO Box C700,West Conshohocken,PA 19428-2959.United StatesThis international standard was developed in accordance with internationally recognized principles on standardization established in the Decision on Principles for theDevelopment of International Standards,Guides and Recommendations issued by the World Trade Organization Technical Barriers to Trade(TBT)Committee.1 electron-hole pairs,one can also express LET as chargedeposited per unit path length(for e

此文档下载收益归作者所有

下载文档
收起
展开