advanced technologyreliability sciences if your address has changed or if you wish to be removed...
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AD-A253 334
RL-TR-92-1 1Final Technical ReportFebruary 1992
ADVANCED TECHNOLOGYCOMPONENT DERATING
DTICAf ELECTE
J U L #0 4 1992Westinghouse Electronic Systems Group ATimothy A. Jennings
APPR1:O VED FOR PUS I, 47LEAS S•" DITR8IUT70N UNIALIM/TED,
92-19900
Rome LaboratoryAir Force Systems Command
Griffiss Air Force Base, NY 13441-5700
. ,..I
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This report has been reviewed by the Rome Laboratory Public Affairs Office(PA) and is releasable to the National Technical Information Service (NTIS), At NTISit will be releasable to the general public, including foreign nations.
RL-TR-92-11 has been reviewed and is approved fcr publication.
APPROVED: ý/Vn14 J~ /A) 51t2TYA4AD
TIMOTHY J. DONOVANProject Engineer
FOR THE GO~mANDER:
JOttN J. BART, Chief ScientistReliability Sciences
If your address has changed or if you wish to be removed from the Rome Laboratorymailing list, or if the addressee is no longer employed by your organization, pl•.asenotify RL( ERS!• ) Griffiss AF!ý, NY 13441-5700. This will assist us in maintaining acurrent mailing list.
Do riot return copies of this report unless contractual obligacions or notices on aspecific document require that it be returned.
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FomApprovedREPORT DOCUMENTATION PAGE MB No. 0704-0188P•Mt mP'l burman my Is ct-lian ai-l ct KUTmra2 Is vsbr• • wavewva in. hs •orww tudnq u'm fto rw ru•vAbwfi hgb-a swd*trg sc• "a sotgaflt-wr n =rrtt ttg l dan r a-wi/ cr qflt - witn rmdwmt, frsca-nn'sutm df kl-muam SfnlCYTTTmrtU r'dw' r, k bsf,• a,-,. s es w a-w c=tw t ,z=e ci its
Dam Hk"wn. Sulm 12 A'fl, u VA =-43= a-td th &m Ofltf d Muugrwt wnda R4 miK Pa•,of PRe±c Pns (O,?04-OW. W0st*q DC 205a
1. AGENCY USE ONLY (Leave Bl.nn. 2-. RPORT DATE a REPORT TYPE AND DATES COVEREDFebruary 1992 Final Jun 89 - Sep 91
4. TITLE AND tiUBTITLE 5. FUNDING NUMBERS
ADVANCED TTCHNOLOGY COMPONENT DERATING C - F30602-89-C-0095PE - 62702F
6. AUTHOR(S) PR - 2338TA - 02
Timothy A. Jennings WU - 4G
7. PERFORMING ORGANIZATION NAME(S) AND ADDRE$S(ES) a PERFORMING ORGANIZATION
Westinghouse Electronic Systems Group REPORT NUMBERFriendship SiteBo:: 746 N/ABaltimore ND 21203
9. SPONSOR!NG/MONITORING AGENCY NAME(S) AND ADDRESS(ES) 10. SPONSORINQ/MONITOHINGAGENCY REPORT NUMBER
Rome Laboratory (ERSR)Griffiss AFB NY 1344L-5700 RL-TR-92-11
11. SUPPLEMENTARY NOTESRome Laboratory Project Enginecr: Timothy J. Donovan/ERSR/(3!5) 330-2608
12a. DISTRIBUT1ON/AVAJLABILfUTY SATEMENT 12b. DISTRIBUTION CODE
Approved for public release; distribution unlimited.
13. ABSTRACTQ.4uun~2m-cThis report has been piepared to sumnaariza the tecbnical study performed to determinethe derating criteria of advanced technology components. The study covered existingcriteria from AFSC Pamphlet 800-27 and the dcvelopment of new criteria based on data,literature searches and the use of advanced technology prediction methods developedin RADC-TR-90-72. The devices that were investigated were: VHSIC, ASIC, MIMIC,Microprocessor, PROM, Power Transistors, P" Pulse Transistors, RF Multi-TransistorPackages, Photo Diodes, Photo Transistors, Jpto--Electronic Couplers, Injection LaserDiodes, LED, Hybrid Deposited Film Resistors, Chip Resistors and Capacitors and SAWdevices. The results of the study are additional derating criteria that extend therange of AFSC Pamphlet 800-27. These data will be transitioned from the report toAFSC Pamphlet 800-27 for use by government and contractor personnel in deratingelectronics systems yielding increased safety nargins and improved system reliability.
14. SUBJECT TERMS i1 NUMBER OF PAGES
Reliability, VHSIC, Galium Arsenide (GaAs), FailurAý Rate, _98De it Ia PRICE CODE_Derat ing ___20____
17. SECURITY CLASSIFICATION 1 a SECJRFIY CLASSIFICAIIOrJ 14. SECURITY CLASSIFICATION 20. UMITATION OF ABSTRACIOF REPORT OF THIS PAGE OF ABSTRACT
UNCLASSIFIED UNCLASSIFIED IUNCLASSWTrED ULNIN 754001 4MStnwo F Brn 298 (Rev 2.89)
Plabo•be by ANSI Ste Z39,162WI 02
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TABIE oF mw=~T
PAGE
1.0 EXECUTIE SLEMQWR 1
1.1 cbjective 1
1.2 Bac]hXmur3 2
1.3 Aproach 3
1.4 List of ALcLonynts 10
2.0 REP01U ORGANIZATICtV 11
3.0 ADVANCED TECI)WGY OXrkNT DERLT1M 12
4.0 N3ICFO=flIJI EERATfl CfLYEINET S 26
4.1 ASIC/VHSi.C Microcircui-t-- 34
4.2 Microprocessor Microcix'dits 58
4.3 amU m4icrocircuits 75
4.4 Application No~teS 87
5.0 NIMMC DEIAW12xG tJID L'MP 89
6.0 POWE TRANSISIOR Dý" ýý CJID=LTS 97
6.1 Silicin Transistors 97
602 Gak.- Transistors 105
3 MF77rs 114
7.0 PF TRANS=XSDZ URýVD rjfG jqý 119
80OPIC-EIX,0MIC1c iF71CE DERATING GJTDELTNES 127
5.0.0 SAW LEMA-T2: G3IDEZIN' 135
211.0 LIERAa'nM VERIFCATON 138
12.3 ALTERNAT APPROC0 TOX SIRýES DER7ITIG 143
13.0 SUMMfvARY 149
14,0 13BT U(ZAMN{ 151Acc:ý,joo Fo,"
Apeudix A DL7RTTNG GUf~I=1iEN EujMMARY r IiS C R4&B SO~~RE I~AD LC lAB
Ju tdIu atoI nce Li
Dit.iu~o ........................ ....... ........ .......
AvWjiabIoitv :c InDis Aw L, Li
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LIST OF 1IUSTlATIONS
FIGURERA
3-1 Fl1ddirt of Technical APNzOac" 14
4-1 C1 Factor for M-X Digital Microcircuits 36
4-2 C1 Factor for Bipolar Digital Microcircuits 37
4-3 C1 Factor for MDS and Bipolar Linear Microcircuits 38
4-4 Package Pin Comnt for M(S Digital Microcirrcuits 39
4-5 Package Pin Oo.int for Bipol3r Digital Microcirc'its 40
4-6 Package Pin Coumt for MS and Bipolar Linear MicrocirQUits 41
4-7 Trasmistor Gate Area for MS Digital and Lliear Microcircults 42
4-8 Dielectric Thickness for Ms Digital and Linear Microcirats 43
4-9 Junctior Tenperature Deratirg for MOS Digital ASIC/VHSIC 44
4-10 Supply Voltage Derating for ?4S Digital ASIC/VHSIC 45
4-11 jurY-iiuii T-a•rc f-r-ti f MVWP_,/Rio!ar Linear ASIC/VHSIC 46
4- 12 Supply Voltage Deratirn for MS Linear ASIC/VHSIC 47
4-13 Junction Tterature Derating for Bipolar Digital ASIC/VHSIC 48
4-14 Criticality Level I SOA for MS Digital ASIC/VHSIC 55
4-15 Criticality Level II SOA for M1S Digital ASIC/VHSIC 56
4-16 Criticality Level III SOA for M4S Digital ASIC/VHSIC 57
4-17 Transistor Gate Area for MOS Digital Microprocessors 61
4-18 Dielectric Thickness for MIS Digital Micropcessors 62
4-19 Junmtimn Torpel-ture Derating for 8-Bit. M)S Digital
MicroProcessomr 63
4-20 Supply Voltage Derating for 8-Bit M1S Digital Microprocessors 64
4-21 Junction Temperature Derating for 16-Bit NOS Digital
Microprooossors 65
4-22 Supply Voltage Derating for 16--Bit MDS Digital Microprooessors 66
4-23 Junction Temperature Derating for 32-Bit NOS Digital
Micrcpracessors 67
4-24 Supply Voltage Derating for 32-Bit m1s Digital Microprocessors 68
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LTST OF I=USTFATIICNS (continued)
FIC&JRE PAGE
4-25 iuwnction Tmperature Derating for 8-Bit Bipolar Micxtcprocessors 69
4-26 Junction Temperature Derdting for 16-Bit Bipolar Microrocessors 70
4-27 Junction Temperature Derating for 32-Bit Bipolar Micrtpropes-ors 71
4-28 C1 Factor for NOS PROIs 76
4-29 C1 Factor Zor Bipolar PRCMs 77
4-30 Dielectric Thickrnes for m s PF4s 79
4-31 Supply Voltag Derating for MSS PRfMs luiiing EEPWA-s 80
4-32 Supply Voltage Derating for EEFRTMs 81
4-33 Write Cycle Derating for E Hs 82
4-34 Maxinum CutTent Density for Microcircuits ep
5-1 MIMIC Failure Rate 93
5-2 MIMIC Prxbability of Suaxcess at 10,000 10L.rs 94
6-1 'ypical ower Transi.-tor SOA 99
6-2 Lifetest Results for GaAs Power MES•FTs 109
6-3 GaAs w MESFET Lifetime. Prediction 110
6-4 On-Off Cycling IAits for Power/RF PiL-se Transistors 118
7-1 CTt--w Innaflcmad ir, an RF Mul~titransistor Packiaae 121
7-2 Assembly Problem Resulting in Thermal Runaway 121
12-1 Ps = 0.9990 SOAs for MS Digital ASIC/VHSIC 146
12-2 Ps = 0.9900 SOAs for MDS Digital ASIC/VHSIC 147
32-3 Ps = 0.9000 SOAs for NOS Digital ASIC/VF.SIC 148
A-I On-Off Cycling Limits for Pawer/RF Pulse Tra¶nstors A-13
liii
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LISr OF TABLES
TABPUI PAGE
1-1 Parts List 1
3-1 ýeratinqr Criteria Approach 153-2 Reliability Me.s and Derating Guidelines Used In Developing
Maxyimm Failure Rates 16
3-3 4axiumm Failure Rates for Each C0-iticaliti• Level 17
_•3•-4 WS Diital ASIC Reliability Model Factors at Derated Values 18
3-5 Reliability K-del Factors arxi Derated Values for ASIC/VHSIC,
flicrc~prxcessors andi P¶R4s 19
3--6 Reliabili ty Model Factors and Derated Values for Silicon
Bipolar Power Transistors 233-7 Gcmieram-mt/MilitarYiIndustry Stress Deratirq Guideline Titles 25
4-1 Attt.ibute and Paramters of Microcircit Model Factors 28
4-2 A';1C,/ ,73IC Device/Strer-Spacific Attributes 34
4-3 ASIC/VSIC IUS Digital Microcircuits Guidelines 50
4-4 M\IC/VHS.TC Bipolar Digital Microcircuits Guidelines 51
4-5 ASIC/VHSIC "VS Linear Microcircuits Guidelines 52
4-6 ASIC/VVWIC Bipolar Digital MicrocircUits Guidelines 53
4-rat-1m; -J--a5
4-8 Micrcpraoesso- Device/Stress-Specific Attributes 58
4-9 MXS Microprocessor Guidelines 72
4-10 Bipoiai Kicimprooesscr Guidelines 73
4-11 Ticroprocessor Stress Derating Criteria 74
4-12 P•g ULvice/Stress-Specific Attributes 75
4-13 WIGS P" Guidelires 83
4-14 Bipolar P"¶* Guidelines 84
4-15 P4M Stress Deratirv, Criteria 86
il
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LISE OF TABLES (orntinued)
TABLE PAME
5-1 Attributes and Paramters of MIMIC Model Factors 91
5-2 NItIIC Device/Stress-Specific Attribtes 92
5-3 MIMIC Stress Deratinr Criteria 95
6-1 Attrijxites and Parameters of Silicon Bipolar PowSr Transistor
Model. Factors 101
6-2 Silicon Bipolar Power Transistor Stress-Specific Attributea 102
6-3 S.lirmr Bipolar Power Transistor Guidelines 103
6-4 Sllicon Bipolar Power •ransistor Stress Derating Criteria 104
6-5 GaAs RVr IMSFET Lifetest Data 106
6-6 GaAs Power Transistor Guidelines 112
6-7 GaAs Power Transistor Stress Derating Criteria 113
6-8 Power SFE Transistor Guidelines 115
6-9 Power MSFELT Stress Derating Criteria 116
7-1 Silicon Bipolar RF Pulse Transistor Guidelines 123
7-2 GaAs RF Pulse Transistor Guidelines 124
7-3 RF Pulse Transistor Stress Derating C-iteria 125
s-1 aito-electric Device Guidelines 128
8-2 Opto-elcctruiic Device Stress Derating CQi•teria 129
9-1 Passive Device Guidelines 132
9-2 Passive Device Stxess Deratirg Criteria 133
10-1 SAW Guidelines 136
10-2 SAW Stress Derating Criteria 137
11-1 Stress Derating Assessment for Level II Criticality 139
11-2 Maxinum Failure Rates for Criticality Level II 140
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1.0 EXECUTIVE SUMMARY
1.1 OBJECTIVE
The objective of this effort was to develop and publish new derating
criteria so that the reliability of new upcoming and modified designs will
be enhanced. Stress deratting parameters were needed for advanced
components such as VHSIC (very high speed ir-cegrated circuits), MIMIC
(microwave/millimeter wave monolithic integrated circuits), GaAs FET
(gallium arsenide field effect transistor), and photonic devices since the
current standards were lacking guidance. The new standards will be used by
hardware design contractors and will serve as the basis, for an update of
AFSC Pamphlet 800-27, "Part Derating Guidelines." The complete parts list
for which updated stress derating criteria was to be developed is shown in
table 1-L
Table 1-1 Parts List
VHSIC RF Pulse .dransistorASIC RF Multi-tb-ansistor~4MIC PackageMicrc~pro-essor Photo Transistor1Rt4 Photo Dicde- ultra-violet erasable Cpto-electronic Coupler- e1ect±rca1ly erasable Injecticn Laser Diode- eleccricalLy alterable UM)- avalanche irduced Hybrid De±posited Film
migration nesistorur~r Transistor Chip Resistor- silic(m Chip Cipacitor- &•As SAW
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1.2 BACKGROUND
Part stress derating has long been established as an imilportant element in
enhancing system reliability. Derating is generally defined as the
practice of limiting electrical, thermal and mechanical stresses on parts
to levels below their specified or proven capabilities in order to provide
a safety margin for operation and to improve system reliability. Most
contractors have developed their own internal derating practices, but until
recently, the DoD (Department of Defense) had no standard practices. RL
recognized the need for standardizing this area. This standardization will
proAide guidance to those contractors without their own policies, indicate
a means for invoking contractual derating requirements and create a
benchmark against which other derating methods may be evaluated.
In keeping with the cost effective tailoring approach to reliability as
defined in MIL--STD-785, "Reliability Programs for Systems and Equipment
Developxm•. nt and P xdutinn Boeing Aerospace (Seattle, WA) under contract
to RL, divided derating cri:t•eria into three different criticality levels.The three level derating approach provides a means of tailoring as a
function ot mission criticality and severity of the end use environment.
RL adapted the results of this study in the publication of AFSC Pamphlet
800-27, "Part Derating Guidedines.'l Further work on derating was performed
by Mart-i Marietta (Orlando, F4• under contract to RL, which included
development of an integrated circuit thermal measurement technique to
verify derating. Both of these eftorts precluded the deve1opment of
der"',Aing 5ctors for new parts dezsigned since the studJ'- were conducted.
While under contract to Pt, Westinghouse rece. '°Ly completed the
"Reliabilit~l At.llysiyA.;sment i:f Advanced Technology" (RA/AAWI) study1
with the intent of updating the microcidrut section of MII-IDBK-217. With
the availability of tJhe stress-failure relationships developed as part ofthat study, as well as ,ose working relationsbips with their :,uppliex s and
available field failure data, Westinghouse was selected to conduct this
"Advanced Technology Component Derating"' study.
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1.3 APPROACH
Stress derating c.' advanced technology components is a critical strp in the
design of rllrctroric sy.stems which e-lnploy these components. Only by the
increased lifetime advantage offered by stress derating can the systera
reliability requirement be reallized wben using advanced technology
components in the system designer's intended application.
It was the intent of the authors of the revised AFSC Pamphlet 800-27 to
maintain the spirit of the current version of the Pamphlet (hereafter
referred to as "the Guidelines") and, at the same time, minimize
unnecessary constraints placed on the designers of electronic systems by
the derating criteria. These unnecessary constraints result from the
application of generalized derating criteria intended to encompass all
components within a specific component style in order to keep the
guidelines simplified. It was believed that, unless the designer can
eimploy derating criteria in his design with minimum difficulty, he will be
reluctant to take the tine necessary to apply the derating criteria
properly. In this day of Total Quality, process streamlining and high
speed design workstations, the designer is motivated to be proactive in all
areas affecting his design. Therefore, in the formulation of the new
stress derating criteria, a change in the derating criteria format is
presented (for microcircuits), with the thought that the designer should,
0.1 AL WLU±U.L J%.LA 1W rIL'.J.L QLKAJUI. LA= C0.JiUk.J1 %J i=L% W.ALt. W LLLýL.L JLA= W QX .Aý .' L C1A,01 IL
be more likely to design an optimum, reliable system by applying the
appropriate stress derating criteria. The need for the change in the
stress derating criteria format was a direct result of the logical approach
taken to update the stress derating criteria, and the structure of the
re-liability modeLs that describe the relationships between applied stresses
and component failures.
It is recognized that the stress derating criteria outlined in the
Guidelines is, by definition, a description of the maximum allowed stresses
that may be applied to a component according to a specified mission
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criticatlity level. It is also recognized that these maximum stresses
result in a maximum component failure rate predicted by accepted
reliability model-,. It is noted here that, at the time the current version
of the Guidelines was released, the accepted reliability models were
ixr)uded in MIL'-HDBK-217D Notice L Therefore, the authors of the current
version of the Guidelines considered the maximum component failure rates,
calculated using the reliability models of MIL-HDBK-217D Notice I and the
maximum stress derating criteria outlined in the current version of the
Guidelines, acceptable for a specified criticality level. A logical
approach to updating this stress derating criteria would be to first
calculate these acceptable maximum component failure rates at each
criticality 'Level. Then, the stress-failure relationships outlined in
updated reliability models, such as those included in MIL-HDBK-217E Notice
1 and the RA/AAT study, may be evaluated such that new maximum stresses
that result in these same maximum failure rates may be identified. These
maximum stresses become the updated stress derating criteria.
This approach to updating the stress derating criteria has (at least) three
benefits. First, the stress trade-offs performed to derive the new maximum
stresses by evaluating the updated reliability models will identify the"lsensitivd' derating parameters in the model that, when varied, result in
the largest changes in expected failure rate. Second, the approach
provides a framework from which derating results can be easily
comraur•c•tci. That t 1-he ornept of how changes in "failure rate" affect
design reliability is more commonly understood among system designers and
reliability engineers than how changes in "percent of rated value" affect
design reliability. Third, the approach provides a basis for evolving the
stress derating criteria into a '1ontinuous" function of criticality rather
than the currently accepted three levels of criticality. This benefit is
expanded upon in a section near the end of this report.
This stress derating approach was applied to several classes of
components. The approach was first successfully applied to microcircuits.
Having just completed the Reliability Analysis/Assessment of Advanced
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Technologies (RA/AAT) study, Westinghouse was intimately aware of those
stress factors which directly influence the reliability of advanced
technology microcircuits. From a study of the RA/AAT results, it was
observed that microcircuit complexity was a "sensitive" derating
parameter. Because of the impact that the complexity of the microcircuit
hal on its failure rate, part of the updated stress derating criteria was
gewerated as simple one variable equations. The variable, of course, was
complexity. For exaorple, in the development of the stress derating
criteria for MOS Digital ASIC/AHSIC cowpormnts, the supply voltage derating
criteria for criticality level . has the form
Si.,pply Voltage = 129 / (G ** 0.320) vclts
where G is the number of gates in the microircuit. In some instances, the
calculated derated stress was virtually independent of complexity. In that
case, a constanL derating value was substituted for the derating equation.
Also, if the calculated derated stress wais ouutide thQe regi- of validity
of the reliability model, the value of the maximum stress identified in the
model was substituted for the derating equation. For example, the maximum
junction temperatures allowed for MOS Digital ASIC/VHSIC level III
compo' ents, although dependent upon complexity, are abc ve the junction
temperatures reoorde,'I in the reliability data used in the development of
the reliability model. Since 125 deg C was the maximum junction
temperature identified in the reliability data, the maximum temperature of
125 deg C is substituted for the de•uating equation.
other microcircuit derating parameters were not explicitly identified in
the reliabilty models. These parameters, such as fanout and frequency,
weze considered design and application attributes which influenced the
dcatabase from which the reliaility models were developed. Therefore, the
updated stress dezating criteria for these parameters were developed froth,
reviews of the literature, supplier information and uther pertinent stxess
derating guidelines.
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A similar stress derating method was used for silicon bipolar power
transistors. Although the MIL-HDBK--217D Nortice I raliability maodel for
silicon bijolar power transistors was significantly differenr from t''e
MIL-HDBK-217E Notice 1 :7eliability model, the approach used in th,-development of the microcircuit derating criteria could be applied co
silicon bipolar power trensistors. The difference between the microcircuit
approach and the silicon bipolar power transistor approach was 0-,at thederating criteria for the power transistor was developed with equal. weightapplied to the stresses identified in the reliability model ofMIL-HDBK-217E Notice 1. That is, the voltage derating and temperatuure
derating for criticality level I must both be 65% of maximum rating so thatthe failure rate calculated using MIL-HDBK-217E Notice 1 would equal thefailure rate calculated using MIL-HDBK-217D Notice 1 (4 FITS). Thetemperature derating was then transformed into temperature unit-s with avalue of 95 deg C (based on a 150 deg C maximum rating). For further de-tails on this calculation, see section 6.1 on page 102.
Since reliabil__ity models for silicon power MOSFETs and GaAs powertransistors were riot available at the time the current version of theGuidelines were published, different approaches were taken to develop
stress derating criteria for these devices.
For power MOSFETs, the, stress dezathig criteria was developed by a tharough
review of the literature and supplier surveys, and consensus of bothmilitary and industry stress derating guidelines. It was deter. ined thatthe currently accepted derating policies ade adequate in themargins of safety and success needed in the intended application.
The stress derating approach for GaAs power transistors was to collectreliability data, develop a stress-failure model and, assuming a maximumfailure rate for each criticality level (provided by R4•, calculata thei. ýximum stresses allowed. This effort resulted in maximum channeltemperatures of 85, 100 and 125 deg C for criticality levels I, II arid II,
respecýtively.
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With the exception that a reliability model was developed on the RA/AAT
study, the stress derating approach for GaAs MIMICs was similar to the
approach for GaAs power transistors. The maximum channel temperatures for
MIMIC devices were calculated to be 90, 130 and 150 deg C for criticality
levels I, II and III, respectively.
It is noted here that, with the exception of the application notes, the
silicon arid GaAs RF pulse transistors are derated similarly to the silicon
and GaAs power transistors si both silicon and GaAs RF pulse transistors
must be able to "dissipate as much power in pulse mode as the silicon and
GaAs power transistors dissipate in continuous mode. GaAs power
transistors (power MESFETs) are often used in RF pulse applications
Opto-electronin components presented a different challenge in developing
updated stress derating guidelines. The differences between the
reliability models of MIL-HDBK-217D Notice 1 and MIL-HDBK-217E Notice 1
res..lted in up to several orders of magnitude difference n in
predicted failure rates. The quality factor had changed 2400% to 7000%,
and the PiT factor of MIL-HDBK-217E Notice 1 utilizes an activation energy
of approximately one third of the activation energy used in MIL-HDBK-217D
Notice 1. The use of the silicon bipolar power transistor approach to
stress derating would have resulted in virtually no stress derating
required to meet thve failure rates that were considered acceptable at the
time the currert version of the Guidelines was released. As an alternative
approach, the development of updated "acceptable" failure rates for the
three criticality levels was considered. The failure rates that can be
obtained by applying currently accepted derating guidelines to the
reliability models were deemed to be as "acceptable" as any other values
chosen. Therefore, without having to do the failure rate calculations and
the reverse stess analysis, the currently accepted guide) ines become the
updated stress derating criteria. A consensus of both military and
industry stress derating guidelines was used in the development of this
criteria.
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There was apparently no change in the reliability models since
MIL-HDBK-217D Notice 1 for the passive components evaluated, namely thlickand thin film resistors, chip capacitors and SAW devices, and therafore
only a consensus of military and industry guidelines was again used in the
development of the stress derating criteria for these components.
To check if the expected results of applying stress derating crite, ia tothe components identified in table 1-1 were obtained, a failure rateanalysis was performed on available field failure data. The analysis wasperformed on field failure data provided by failure databases from the
AI/APG-66 and AN/APG-68 radar programs and the ALW-131 radar jammer programduring the sorties flown in the 1988 and 1989 time period. It wasdisoovered that che failure rates for PROM4 devices, power transistors, RFtransistors, epto-coupler.,-, LEDs and thin film chip resistors were close to
or below the failure rate that- would be expected when applying the stressderating criteri .- outlined in the current version of the Guidelines. Onlythick PIm resistors and cxramic chIp capacitors experienced failure rates
significantly above expected failure rates. The most likely reason forthis discaepancy" is that these components often get removed as part of the
reworx for the suspected failure of another component. Since failureana2~lyss are typically not. p-rformed on most of the components removed from
system~s, it is quite possible that some of the "failed" components are not
truly failed. The calculated failure rates in this analysis would
there•ore be inflated. The rcsults of this verification analysis are, in
either case, most encoura,9isg.
At the completion of this study, one concern is still left unresolved. Theconcern is -dhat the designer is 'locked ir." to a level of derating criteria
based on mission type of the whole isystem (SF, AUF or GF, for example)rather than the true component or board criticality. This concern
prompted the authors of this study to include a section near the end of
this report which outlines an alternate approach to implementing stressderating guideli es. The intent of this approach was to justify the
PasonihAlenrss of imnposing criticality level I guidelines on a criticality
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2evel III mission design, and vice versa, depending as much upon systemarcldtecture. s the safety ard success of the mission. The possibility ofevolving stress derating criteria into a "continurous" function ofcriticality is evaluated.
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1.4 LIST OF ACRONYMS
The following is a list of the acronyms used in this report.
AFSC - Air Force Systems Command
APD - Avalanche Photo Diode
ASIC - Application Specific Integrated Circuit
ATCD - Advanced Technology Component Derating
CTR - Current Transfer Ratio
EEPROM - Electrically Erasable Programmable Read-Only Memory
EM - Electromigration
ESD - Electrostatic Disrharge
eV - Electron Volt
FET - Field Effect Transistor
FMEA - Failure Modes and Effects Analysis
FPMH - Failures Per Million Hours
GaAs - Gallium Arsenide
ILD - Injection Laser Diode
JFET - Junction Field Effect Transistor
LED - Light Emitting Diode
MESFET - Metal Semiconductor Field Effect Transistor
MIL-HDSK - Military Handbook
MIMIC - Microwave/Millimeter Wave Integrated Circuit
MOS - Metal Oxide Semiconductor
MOSFET - Metal Oxide Semiconductor Field Effect Tran'sistor
PROM - Programmable Read-Only Memory
RA/AAT - Reliability Analysis/Assessment of Advanced Technologies
RL - Rome Laboratory
RTOK - Retest Okay
SAW - Surface Acoustic Wave
SOA - Safe Operating Area
TDDB - Time Dependent Dielectric Breakdown
VHSIC - Very High Speed Integrated Circuit
VISI - Very Large Scale Integration
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2.0 REPORT ORGANIZATION
Section 3.0 presents the three approaches taken in the development of theupdated stress derating criteria. Each approach is outlined briefly in
this section with the details of the approaches provided in the followingseven section No stress derating criteria is developed in this section.
Section 4.0, 5.0, 6.0, 7.0, 8.0, 9.0 and 10.0 discuss silicon
microcircuits, MIMIC device-s, power transistors, RF tran.irtors,
opto-electronic devices, passive, components and SAW devices, respectively.
Stress derating cz-i'eria and associated application notes are provided in
each section for the relevant components in that section.
Section 1.o presents a summary of the accumulated field failure data for
the available component types outlined in table 1-1. A comparison of thepredicted failure rate based on Level II criticality derating and the
observed failure rate is made to ve'-ify the accuracy of the stress aerating
criteria.
Section 12.0 discusses an alternate approach to stress derating derived
from observations made in the development of the updated stress derating
criteria for this study.
Section 13.0 summarizes the results of the study and presents conclusions
and recommendations for follow-on analysis.
cSection 14.0 contains the bibliography of the literature used in part to
develop the updated stress derating criteria.
Appendix A provides a comprehensz.ve sulm-ory of the updated stress derating
criteria and associated application notes.
Appendix B provides sample Fortran programs used in the development ofstress derating criteria for microcircuits.
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3.0 ADVANCED TECHNOLOGY COMPONENT DERATING
The developrent of stress derating criteria for advanced technologycomponents requires a fundamentally sound understanding of the
relationships between the electrical, thermal and mechanical stressesapplied to the components and the resultinq life distributions of the
component populations. Component reliability models ara used to describethese relationships and provide insight into the functional dependence of
component life distributions on the applied stresses.
The magnitude of the stress derating determines the amount of expectedchange in component lifetime or shift in the life distribution of a
population of components. In general the more the stress is derated, the
longer the life of the component. Therefore, the expected result of
derating the stresses applied to a component is to decrease its failurerate. Since most reliability models relate electrical, thermal and
mechanical staesses to component litetime in tie fociz, of a fai2-uro rate, itis reasonable to use the concept of failure rate as the key link between
the reliability model and the stress derating criteria.
The minimum acceptable stress derating depends upon the criticality of themission. Criticality levels referenced to mission safety and success, as
outlined in the current version of the Guidelines, can be established and
contasted -in terms of failure rates. The minimum acceptable stress
derating for each criticality level sets the maximum failure rate that
might be experienced by the component in a mission of specified
criticality. It is reasonable to maximize the stress derating, when
possible, to provide a greater than minimum margin of safety and success.
The definitions of the criticality levels used in the updated version of
the Guidelines are consistent with the current version of the Guidelines.
It is noted, however, that the formulation of the updated .tress deratingcriteria is iriven by the component failure rates associated with eachcriticality level and not solely the definitions of criticality.
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Criticality Level I (.':aximum Derating). Used with equipment whose
failure would substantially jeopardize the life of personnel,
would seriously jeopardize the operational mission, or would
require repairs that are infeasible or economically unjustified,
or used when extremely high operational readiness requirements
are specie~ed. Level I derating is considered those stress
levels below which further reliability gain is small or at which
further derating will create design problems that are
unacceptable. This level is intended for the most critical
applications in which design difficulty can be justified by Lhe
reliability requirement.
Criticality Level In Used with equipment whose failure would degrade
the operational mission or would result in unjustifiable repair
costs, or used when high operational readiness requirements are
specified. Level II derating is considered still in the range in
which reiiabality Ya-"n5 adr rapid u trA-esiS i5 deca eased.
However, achieving designs with these reductions in allowed
stress is significantly more difficult than at level III.
Criticality Level III. Used with equipment of lesser criticality than
level I or II, namely, equipment whose failure may not jeopardize
the operational mission or that can be quickly and economically
repaired. Level III derating is that stress level reduction that
causes minor design difficulties and yet generates a large
incremental reliability gain. The large reliability gain is
realized since the effects of stress increase greatly as the
absolute maximum rating is approached.
Supplemented by updated stress-failure data provided by three sources,
namely, a thorough review of the literature, evaluation of available field
data and component supplier surveys, the component reliability models
developed on the RL "Reliability Analysis/Assessment of Advanced
Technologies" (FA/AAT) and "Reliability Prediction Models for Discrete
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Semiconductors" 1 69 studies provided a starting point for the developmentof the updated stress derating criteria for several of the component types
identified in table 1-L For those component types not covered by currentreliability models, stress derating criteria was developed from eitherreliability models generated from accumulated life test data or fromconsensus of current stress derating guidelines available frov multiplemilitary and industry sources. These approaches to understanding thestress-failure relationships of advanoed technology components, outlined infigure 3-1, were executed on a priority basis in the order listed above.That is, if a current reliability model was available, it was used(approach A). If a reliability model was not available, a reliability
model was developed, when possible, from accumulated stress-failure data
Device List7Ij•J
SKevword List ].WEC Part NumberZ
Vendor Visit] Vendor Contacts F Systen identity
FTheory L ldp3 • rE[I.her ,L~per-~~d L~pr Field Fatr Fiel
Strnss / Failure Dai.gbase hicluding Application Limitations
J 8. Develop ,Vodel]
L Stress/ FilureRelationships - A. Rel. Models
Derating C.itcria - C. Derating Guidelinels
Criteria Verification]
Figure 3-1 Flowchart of Technical Approach
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(approach B). If it was not possible to develop a reliability model, then
a consensus of available derating guidelines was used to generate the
proposed derating criteria (approach CQ. Table 3-1 identifies the approach
used for each component type listed in table 1-1.
In the approach taken to update the stress derating criteria using
rel/ability models, approach A, a methodology was established in which a
maximum failure rate was calculated for each criticality level for each
component type. The reliability model used to generate these maximum
failure rates was MIL-HDBK-217D Notice 1, since this revision of
MIL-HDBK-217 was the current Handbook revision (13 June 1983) at the time
in which the current version of the Guidelines was released (5 December
Table 3-1 Derating Criteria Approach
"I- ?nN- - - I- I
ASIC A, CWisIC A,CMicroprocessor A, CPRCM A,CMIMIC A,CPower Transistor A,B,CRF Pulse Transistor CRF Multi-tLansistor Package CIPhoto Transistor CPhoto Diode COpto-electronic Coupler CInjection Laser Diode CLED CHybrid Deposited Film Resistor XChip Resistor CChip Capacitor CSAW C
KEY: A - Reliability Model AvailableB - New Reliability Model DevelopedC - Ccocensus of Available Derating GuidelinesX - Insufficient Lnformation
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1983>. The reliability models and derating guid lines used to calcui.ate
the failure rates are shown in table 3-2 for each component type for which
approach A was used. These failure rates, listed in table 3-3, represent
the maximum failure. 1ates expected for the given criticality level allowed
by the current version of the Guidelines.
The example of how the stress derating criteria was applied in the
development of the maximum failure rates for MOS digital ASIC/ VkSIC
microcircuits is shown in table 3-4. Using the stress derating criteria
for eiOS mirocircuits in the current Guidelines, the maximum values of each
factor in the reliability model were determined for each criticality
level. The failure rates were calculated to be 0.3402, 3.0593 and 31.640
fpmh for" criticality levels I, II and III, respectively (see table 3-3).
Table 3-2 Reliability Models and Derating GuidelinesUsed In Developing Maximum Failure Rates
Component Type NIIrIIDBK-217D Notice I AFSCP 800-27 (1983)
ASIC/VHSIC Microcircuits: Microcircuits:- MS Digital - Mownlithic MOS Random Logic ISI Digital (MJS)- M4S Linear - Monolithic MOS Linear - ldnear (MOS)- Bipolar Digital - Mrnolithic Bipolar Ran. Logic LSI -. Digital (Bipolar)- Bipolar Linear - Mnolithic Bipolar Linear - Linear (Bipolar)
Miczprocessor Microcirc•its: Microcircuits:- __ - Microprocessor (MrS) - Digital (MVS)- Bipolar - Microprocessor (Bipolar) - Digital "Bpoar
P" Microcircuits: Microcircuits:- MS - PRM (S) - Digital (MlG)- Bipolar - PRM (Bipolar) - Digital (Bipolar)
Power Transistors Transistors: Transistors:- Silicon Bipolar - Group I, Silicon - Bipolar Silicon- GaAs - (Not Listed) - Field Effect- MDSFEr - (Not Listed) - Field Effect
1.6
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Table 3-3 Maximum Failure Rates for Each Criticality Level
Failure Rates (fmih) for Levels:
Component Type I II III
ASIC/VInsIC- NOS Digital 0.3402 3.0593 31.6405- NOS Linear 0.4932 4.3920 46.0962- Bipolar Digital 0.3126 1.5862 11.6614
Bipolar Linear 0.4932 2.7477 24.8862
Micrcprocessor- NOS 0.3402 3.0593 31.6405- Bipolar 0.3126 1.5862 11.6614
PROM- NOYS 2.7371 22.7459 264.2236- Bipolar 0.6322 2.8023 23.6754
Power Transistor- Silicon Bipolar 0.0040 1.2917 0.5763
The reliability model parameters and derating values for the microcircuitsand power transistors for which approach A was used are shown inabbreviated format in tables 3-5 and 3-6, respectively. The calculatedmaximum failure rates "bound" the stresses driving the componentreliability, described by the updated component reliability models, suchthat these maximum failure rates could not be exceeded. The values of thestresses, in absolute form or as a percentage of the maximum rated value,became the new derating criteria. Using this methodology, the new deratingcriteria could remain consistent with the old derating criteria. That is,the updated stress derating criteria will not allow a component to be usedin a particular mission with a higher failure rate than was allowed by thecurrent version of the Guidelines. In fact, the derating criteriadeveloped for more complex microcircuits results in a lower failhre rateper function for these microcircuits than less complex microcircuits. It
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Table 3-4 MOS Digital ASIC Reliabihity Model Factors at Derated Values
Level Factor Value Stress Derating AttriLbites
I PiQ 0.5 S levelI PiT 6.9 85 deg C, A = 7532I PiV 1.0 5 voltsI PiE 0.9 SFI PiL 1.0 > 4 mnths productionI Cl 0.0919 20,000 GatesI C2 0.0024 20,000 GatesI C3 0.048 64 pin DIP, glass seal
II PiQ 1.0 B LevelII PiT 16.1 100 deg C, A = 7532II PiV 1.76 12-15.5 volts, 85% derating, 100 deg CII PiE 9.0 AUFII PiL 1.0 > 4 months productionII C1 0.0919 20,000 GatesII C2 0.0024 20,000 GatesIi C3 0.048 64 pin DIP, glass seal
Il PiQ 6.5 B-2 LevelIII PiT 27.3 110 deg C, A = 7532III PiV 1.89 12-15.5 volts, 85% derating, 110 deg CIII PiE 2.5 GFIII PiL 1.0 > 4 months pr:i/uctionIII C1 0.0919 20,000 GatesIII C2 0.0024 20,000 GatesIII C3 0.048 64 pin DIP, glass seal
is noted here that the environmental factors were chosen for the saruereason other constants and parameters were chosen, that is, to give themaximum failure rates. It should be noted, however, that the value of the
worst case environmental factor (as well as the other factors) in the
development of the maximum failure rate cancels with the worst caseenvironmental factor (as well as the other factors) in the development ofthe updated stress derating criteria. Again, the intent was not to develop"Conservative,, results, but results that would be. considered commensurate
with the results already experienced when using tht stress deratingcriteria outlined by the current version of the Guidelines.
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Table 3-5 Reliability Model Factors arid Derated Valuesfor ASIC/VHISIC, Microprocessors and PROMs
a aa4K -I K 6K K 4K-K-
4O) a 0 QO 0 0 . 00
a. a a 0ý C' o ;C a a3 aD
"51 4m a, anC m aC , C 5C3 C DC 3C 3 4 a
C>3 cta- ,@~4 0 0 0 a0- CDl * 000 *ý c-al 000
-' r4 In 4.-e fn -rm an C l
*~- 4 *a
ad, a- 44 * a2aL-c *F-0 a g 'a r - c *et r c . 0
2 3 ~ pt :0 za :U Q'-i*O M 0 - ).U ~CI- ~ ~ ~ ~ ~ ~ ~ n '0'O a C0-*N 4 'o-*0O' '-t-*''? a'
CU * C'.ja a ~ aa .CJ a . ~ Q6
4 4 4 a 19
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Table 3-5 Reliability Model Factors and Derated Values forASIC/VIISIC, Microprocessors arid PROMs (continued)
ai C4 -4 aa ?A a )(
- 0 C~O a iJO, C I= J 0 -C3 b! C31 Im 0 0 C3J C.- V.0 -af C$ C
m 1t'0 FQQ ~ In~ a 0CQ ae4 = a 10 C1 0Q~'
m CI 0 1~ f C a.O * 0,. Cm Q J.t aQ 00.- C 01 e - C6~~ a1 0CJ1
W 2S .Iim a z307 C18 a a 1 " 0 a CI ZI a1 1 I -1CS Cc. aý 0 0 a; a; aD aý0 C ; ý C - ~
0 C!. a. . a. . a9 . a.999 9 .4 C n C a 0 CD aýO a a aD aD C j M 0C 0C
0 0a
*) aj at a a1 J a
do X am 3 . a a
a a a a a0
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Table 3-5 ReliabiliLty Model Factors and berated Values forASIC/VHSIC, Microprocessors and PROMS (continued)
00- 4a 00- LA Ul 4L.-44
it 4 4 4 ir. 4 'A~ 4AL
&A 4 A 6A 'A 4 W
fm 44 4q 4v -t -. 4y -~ CU-ct
*. cc c wnvq~sc
n icO(J J J it, r-r &--1C1 ..
riI. " -C -C. 1- -K N.z r- Z Z -K - C. -C -C 1-C->> * >> ~~4C ~ % > ~ t > 4 .
l~u 4 BA.) 4 ; C; C; L; M 4; 4; C L;
S/l~fl ; U~l 4 4; Wtl l 4 4 . 0
EC) NN. C3 C3 NCe C3 NOInCD
44n r- I4-" H m l I I r- ~ tI r- *ICI N ! - =il .- ils
'00 8 0mt>a3 5 40 OLI ) -00) 0 4 M0 *A i0 n 4 .0CD~~~~ ~ ~ ~ C>C ,SC 00ýC 1n O
to- Wcc toc In00400n3C CAcc W toC.CA w, lW,43- 0-24 4a -on (0344 t.*( 304300 w 4
-0 * C9.. . -- C
43 4 4 ~4 44
~~0~ 0N0 N. N. N' (A N N
&1 4 C I m 4' y_ 4- U 4 ' f 4 4
211
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Table 3-5 Reliability Model Factors and Derated Values forASIC/VHS2EC, Microprocessors and PROMs (continued)
0 ~ ~ t $A fA 'A CA 'A 4 0 0 CO m 0 0 'A m W
4., 4.4 44. 4.- 41.4 .1~41'4a 44 4 4'4 4s 44 - 1'
: a. .1 . 4 4 4. 4.aa
A AA A AA 'A A A A A AA A A A~ A A A A A A A A
4-a w L Id 44 )4 ) 4 4 0 V q) C; 4 43 4 W 0 IV4
(A * C 4 U4 w 0 40 )# )wm 4 4 U)# AV
C24 4. a0 42 Cm (2 C 0 00C
13013 9 13 CA 9 L.9L a 0333111.11. 3136 .13131A.1a-3G0. 0. - I
0) 40 al ' nE E n 'Al fn i nEnE n 0n fA 0) 'A En 4, 4,E n * i nE
U 00), 300 ,ZUIl 40, UO 120 a42 Q0 C2 0(5 A A7
C. P ( . CD C0 C.3 000 C 00 C 00 3 C)0 C) C)0 D C) C) nL " f nIK. M. M. (N CU a. a. fn.a ~ .a . a. a. . . a. .a *a..a .a.a
-J41 ' 4
OW .,*IZ- at x50 m 4-.4.. 4O 0(50 *
-aJ 13- 4~ fn a - i4 Pn a4.--M.
L3. 4~ r
U 01 4 .4
I-______ -A______ L._____9C
>< -* a,' N a~43*'N3* E'l' EI'di 1- 4 4041- 1 U5 .. .
9-. m9 SW -l4- -.- L '.3 4.3 'N a4 '(.3 N .N ara
223
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Table 3-6 Reliability Model Factors and Derated Values forSilicon Bipolar Power Transistors
Description Factors
Device Prediction Crit. Base FR Quality I Cowdi2xity Env*,onmentType Reference Level (LambdaB) (PiQ) (0l) (A'IE)
Transistor MIL-217D1 1 0.0092 0.12 1.0000 0.40Group 1 2 0.0092 0.24 1.0000 65.00(Silicon) - 3 0.0092 1.20 1.0000 5.8,
Description Factors Failure Rate
Device Prediction Crit. Application Power Rating Volt. Stress (Failures IType Reference Level (PiA) (PiR) (PiS) 10-6 Hrs)
Transistor MIL-217D1 1 1.50 5.00 1.20 0.0040G r o - ',! 1 .5 0 5 1 . . .1, r 5.0.0 1.0 1 ,(Silicon) j _ 1.50 5.00 1.20 0.5763
Description Rationale
Device Prediction Crit. Base FR Quality Complexity EnvironmentType Reference Level (LaenidaB) (PiG) (C0) (PIE)
Transistor HIL-ZfD1 M 1 (Rax) JANTXV singie Trans. SFGruup 1 2 (max) JANTX Single Trans. AUF(Silicon) 3 (max) JAN Single Trans. GF
Description
Device Prediction Crit. Application Power Rating Volt. StressType Reference Level (PiA) (PiR) (PiS)
Trans;stor MIL-217D1 1 Linear 200 Watts S2 - 70%Group 1 2 Linear 200 Watts $2 a 70%(Silicon) 3 Linear 200 Watts s2 u 70%
23
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In the approach to update the stress derating criteria by creating new
reliability models, approach B, stress-failure data accumulated from the
literature search and supplier surveys wa., examined, and the r"eliability
model was generated, It is noted here that this approach was used only for
the temperature parameter in the reliability model for GaAs power
transistors (see Section 6.2).
If approaches A and B were not viable, then a consensus of available
derating guidelines was used to update the stress derating criteria,
approach C. The fourteen guidelines used in the criteria development are
listed in table 3-7. Of these fourteen guidelines, twelve guidelines were
from government or military sources and two were from industry sources.
V parameters selected for derating by these fourteen sources were not
consistent between the sources. Therefore, before the stress derating
criteria could be evaluated, it was first necessary to identify the key
-rarmeters to be derated. These key parameters were initially limited by
ttie sources that specified derating criteria for three criticality levels
(guidel ines A through F). The remaining parameters were included as
application notes, when appropriate. It is noted here that guidelines A
anid B were exactly the same, and therefore, guidelines A and b were
considered one source in the development of the final updated stress
dexating criteria. Once these parameters were identified, the consensus of
the five guidelines was obtained by calculating the median of the stress
dorý.Ung values for each stress parameter.
Ln.Ul cases, application notes and design limitations were developed from
accwu-Wtd component information, obtained in the literature search or
-.•d r. surveys, and extrapolated from other derating guidelines. The
ao~'9[Lr• notes for each component type are furnished at the end of each
py.v-i'c' :Leport sections and in Appendix A. In addition, the adequacy of
.Z ivress derating criteria was reviewed using failure rates calculated
ftom awcumulated field failure data (see Section 11.0).
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Tah-Ile 3-7 Goverrunent/IMilitaxy/Industry Stress Derating Guidel-ine Titles
Designator Guideline
A AR3C Paniphlet 800-27, 5 Deoe1*er 3,983B FS-TR-83-197C ESD-'M-85-148D RAD)C-M-84--254E RADC-'M-82-177F NASC AS-4613G GSFC PPL-18 (MNSA) , October 1986H NAVNAT P-4855-1AJ MILrSfl>2174 (AS), July 1976F !4Th-SID-75H (NA&X) , June 1989If NAVSEA TEOOO-AB-GIP-010, September 1985M M~r-gID--1547A, Dwarber 1987W OFM Ax OEM B
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4.0 MICROCIRCUJIT DERATING GUIDELINES
For advanced technology silicon microcircuits, the RA/AAT reliability
modelsI can be summarized in general form by
L(to) = PiQ * (Cl * PiT + LCyC + C2 * PiE) * PiL + LTDDB (to)
+ LEM (tr), ()
where:
I4to) is the device failure rate at time to in failures per million
hours,
PiQ is the quality factor,
PiT is the temperature acceleration factor, based on technology,
PiE is the application environment factor
PiL is the learning factor,
C1 is the circuit complexity failure rate in failures per million
hours,
C2 is the package complexity failure ratsA in failures per million
hours,
LCyc is the EEPROM write cycling induced failure rate in
failures per million hours,
LTDDB(to) is the time dependent dielectric breakdown (TDDB)failure rate at time to in failures per million hours, and
l;M(to) in the electromigration (EM) failure rate at time to in
failures per million hours.
A review of the literature 2 9 -1 0 0 concerned with microcircuit failure,
during the time since the RA/AAT reliability models were generated,
resulted in no change to thce basic rcliability models. However, it was
noted that, since failures due to electromigration, having failure rates
LE., are distributed normally with the logarithm of time with very small
variances, the effect of LEM on the total failure rate, L(to), is
either negligible or catastrophic. Therefore, the Lim term was
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eliminated from the equation for calculating failure rate and the
,•ectromigration effect is presented as an application note. Without this
LM term, the failure rate equation for deriving stress derating criteria
simpliiile to
L(to) = PiQ A (C1 * PiT + Lcyc + C. * PiE) * PiL + LTDDDB (to) (2)
The stress parameters and attributes that directly affect the calculated
failure rate for a siiawn microcircuit are embedded in the Pi, complexity,
and wear out failure rate factors of the reliability model. To extract the
maximum stresses allowed for each criticality level from the factors in the
reliability model, L(to) in equation (2) must be set to the maximum
failure rate allowed by each criticality level. These maximum failure
rates are specified in table 3-3. In the approach to develop stress
derating criteria for advanced technology sill'con auicrocircuits, the
parameters and attributes of the failure rate model factors were separatedintothre goup,aon group for ~~j.'ij /C ~.u4e
group for device-specific (DS) attxibutes and the other group for
stress-specific (SS) parameters. Table 4-1 outlines the relationship
between the factors in the failure rate equation, the distinction between
criticality-specific, device-specific and stress-specific parameters and
attributes associated with the factors, and the microcircuit technologies
for which these parameters and attributes are applicable.
There were two basic types of device-specific attributes, technology and
complexity. The technology attribute was handled by creating stress
derating criteria for each technology individually. For exaiiple, there are
digital and linear, MOS and bipolar ASIC/VHSIC microcircuits. Therefore,
four stress derating tables were developed, one for digital MOS ASIC/VHSIC
microcircuits, one for digital bipolar ASIC/VHSIC microcircuits, one for
linear MOS ASIC/VHSIC microcircuits and one for linear bipolar ASIC/VHSIC
microcircuits. The complexity attribute was handled by making the circuit
complexity parameter (i.e., number of gates, transistors or bits) a
variable in tlh stress derating criteria. Because of the large number of
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Table 4-1 Attributes and Parameters ot Microcircuit Model Factors
Application to:
Factor Type Attribute / Parameter MOS Bipolar
PiQ CS Application Envixorment Y Y
PiT DS Technology Y Y
Ss Junction Temerature Y Y
PiE CS Application Envitoiment Y Y
PIJL CS Years In Production Y Y
Cl DS Circuit Technology Y YDrn Circuit CmPleRxity Y Y
C2 Ds Package Tecluology Y YDS Package C~mplexity Y Y
L CYC DS Circuit Opeiity I Y * NSS Number of Write Cycles Y * N
L TDDB DS Circuit Cmplexity Y NSS Juncticn Tempet-a-ture Y NSS Supply Voltage Y N
KEY: * - O Only
Computations reqUred, the C1 factor tables in the RA/AAT final. report were
transformed to continuous functions. A relationship between circuit
oamplexity and package comRlexity was developed from literature sources 5 7
such that the package complexity parameter (i.e., number of pins) could
also be handled in terms of the circuit complexity parameter. All other
rx4lationships required in the development of the derating criteria were
also based on cixuit complexity. It js noted here that all relationships
based on circuit complexity were always developed in a conservative fashion
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such that the resulting stress derating criteria would be valid for all
complexities of microcircuits.
The criticality-specific attributes included the application environm'ent
attribute and the years-in-production attribute. The application
environments for the PiQ factor were always S-Level, B-Level and B-Level
for criticality levels I, II and III, respectively. The application
environments for the PiE factor were always SF, AU and GF. for
criticality levels I, II and III, respectively. These application
environments were chosen since they were the most closely related to the
application environments outlined by the criticality levels in the current
version of the Guidelines and resulted in the highest failure rate for the
criticality level they represented. The years-in-production attribute for
the experience factor, PiL, were always 2 years, I year and 0.75 years for
criticality levels I, II and III, respectively. These years in production
were chosen based upon current experience with component procurement for
systems that can be categorized by the definitions given for each
critical.ty level.
The stress-specific parm-meters, as mentioned previously, are the only ones
that, when changed, re ;ult in a different failure rate for any given
microcircuit. These parameters, temperature, voltage and number of write
cycl, (EEPROMs only), are the ones that can be traded-off to obtain the
're- f-'1m- r fn.r A ...iva ...i.n... ....iiit. A -as-nnn..ra h
was taken (with an exception for EEPROMs, see Section 4.3) in developing
the bounds for these stress-specific parameters such that the resulting
derating criteria would be effective, but not oppressive, in the desired
application.
This approach initially ignored the number of write cycles, or LCYC,
which was only applicable to EEPROMs. It was then assumed that, if the
time dependent dielectric brea&iý.dwn (TDDB) failure rate was not a factor
because wear out was not a concern, then the only s-tress-specific parameter
left was temperature. .t is noted here that the defect -related failure
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rate (exponential probability density function) is a concern for allmicrocircuits and cannot be ignored. The independence of the TDDB-drivenwear out stresses and temperature is addressed in Section 4.1 in theexample of MOS digital ASIC/VHSIC microcircuits. For any microcircuit of agiven complexity, the temperature was calculated for which the failure rate
did not exceed the maximum failure rate given in table 3-3, dependent uponcriticality level. In calculating this maximum temperature, it was noted
that the maximum failure rate was not always the limiting factor. Becauseof the form of the failure rate equation, to solve for temperature imbedded
in the PiT factor rf-piired the term L(to)/(PiQ*PiIQ to be greater thanC2*PiE. Since L(to), PiQ, PiL and PiE are fixed for a given type ofmicrxcircuit, C2 controls the validity of the argument. For this reason,only microcircuits of a specified maximum complexity are acceptable in a
given criticality level. This complexity limit is included in the stressderating criteria for microcircuits when applicable. If the maximum
temperature was calculated to be a value higher than 175 degrees Celsius,
then 175 degrees Celsiut was c1h.sen. as the ma."'mum temperature.
Once the maximum temperature had been calculated for a microcircuit ofgiven complexity, it was noted that any operating teimperature below this
maximum temperature resulted in a calculated failure rate that was lessthan the maximum failure rate allowed by the criticality level. This
difference in failure rate could then be used to bound the stresses
associated with tie TDDB wear out mechanism. Table 4-i shows TDDB failurerates are only applicable to MOS microcircuits, and therefore, this
development of the derating criteria for supply current is only applicable
to MOS microcircuits.
Time dependent dielectric breakdown is a failure mechanism that results in
a component failure distribution that is normal with the logarithm oftime. That is, unlike the failure rates currently addressed by1MIL-HDBK-217 Revision E Notice 1, the TDDB failure rate is timedependentI. There are three factors that affect the rate of failure forTDDB, the electric field across the dielectric, the dielectric film
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temperature and the total area taken up by the transistor gates. A
relationship was also developedI between the latter factor andmicrocircuit complexity. When dealing with a failure rate model thatincludes LTDDB, it is assumed that the dielectric film temperature is the
same as the junction temperature defining the PiT factor. Therefore, wit.h
th& film temperature previously defired and the total transistor gate area
correlated to microcircuit complexity, the only factor that is not defined
is the electric field.
This electric field factor is proportional to the supply voltage accordingthe dielectric thickness Mhich is related to the complexity of the
microcircuit. The difference in failure rate between the maximum deratedtemperature and the operating temperature therefore defines the maximum
derating criteria for the supply voltage. That is, with the operating
junction temperature less than the maximum junction temperature, theresulting failure rate is less than the maximum failure rate allowed by the
criticality level. Therefore, the microcircuit could be operated with asupply voltage higber than the supply voltage allowed when operating at the
maximum junction temperature provided the maximum failure rate is not
exceeded.
With the device-specific, criticality-specific and stress-specific
attributes and parameters defined, the maximum junction temperature and
maximum supply voltage (MOS microcircuits only) derating criteria was
developed. For convenience in developing this derating criteria, softwareproTrams were written in FORTRAN 77 programming language. Appendix B
contains an example program written to calculate the temperature and
voltage values displayed in the graphs for MOS digital ASIC/VHSIC
mxicrcircuits. Once the derating values were calculated, a least squares
fit transformed this data into simplified equations dependent upon circuit
complexity. The simplified equations become the update stress derating
criteria for thie junction temperature and supply voltage stress parameters.
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It is noted here that, in some instances, the calculated derated stress was
virtually independent of complexity. In that case, a constant derating
value was substituted for the derating equation. Also, if the calculated
derated stress was outside the region of validity of the reliability model,
the value of the maximum stress identified in the model was substituted for
the derating equation. For microcircuits, it was determined that the
applicable reliability models were based on junction temperature data that
did not exceed 125 deg C. Therefore, this maximum junction temperature was
used in those cases where the calculated derated junction temperature
stress was above 125 deg C. It is also noted that the microcircuit
reliability models outlined in the RA/AAT study were valid only up to a
specified maximum complexity. Although the data graphs generated and the
corresponding stress derating equations are continuous past the specified
maximum complexity, the stress derating criteria is not considered valid
beyond this maximum complexity. Therefore, the derating parameter of
"maximum complexity" is included in the list of derating parameters for
microcircuits.
since existing stress derating guidelines, other than those for the
stresses explicitly identified in the reliubility models, have purposely
affected the observed failure rates of components used in applications
corresponding to one of the three criticality levels, it was necessary to
review the existing stress derating guidelines to determine their relevance
in being included in the updated stress derating guidelines, given that the
factors being derated were not explicitly included in the current
reliability models. It was observed that failure data for components that
did not abide by the stress derating criteria war not readily available
(typically due to goverment or military contracts that require some type
of derating) and to arbitrarily remove this criteria may be irresponsible.
Therepore, the updated stress derating criteria for microcircuits includes
both the n-awly created criteria baced upon updated failure rate models as
well as the current criteria which was developed for parameters not
explicitly included in the updated failure rate models. It is noted here
that the only stress derating criteria included by the guideline sources
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that outline three criticality levels were included n this proposed
revision of the Guidelines.
TI\ application notes for advanced technology microcircuits were developed
from a review of applicable literature, supplier surveys and other stress
derating glidelines. These application notes may be found at the end of
this microcircuit section and in Appendix A.
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4.1 ASIC/"VHSIC MJICROCIRCUITS
ecause of differences in technjology within the ASIC/1 HS C category, stress
derating tables were developed for KoS digital, bipolar digital, MOS
linear, and bipolar linear ASIC/VHSIC micro-dircuits. The differences
between the criteria in each table were the results o.1 applying the
different davice-spealfic attributes and stresa-spe-eifc parmeters to the
failure rate equation. These attribute" and paxameters included
temperature activation energy (PiT), circuit comp:lexity (Cl), number." of
package pins (C2), total tý.nsistor gate area (LTDDB) and dielectric
thickness (LTDDB), Table 4-2 outlinA-s the values or equations used in
evaluating these_ device/stress-specific attributes.
Table 4-2 ASIC/VHSIC Device/Stress-Specific Attributes
Te±mnology I Attribute Value / Equation
MOS Digital Ea 0.35 eVCl 0.01 + 0.00042? * GATES *w 0.588Pins 11.07 * GATES ** 0.342C2 2.8E-4 * IINS ** 1.08Transistor Gate Area 1349 * TRANS ** 0.609 (sq umn)Dielectric Uidckness 4.93 / A * 0.266 (kA.)
Bipolar Digital Ea 0.60 eVCL 0.0025 + 0.0000977 * CATES ** 0.601x -'-- 9.16 * C-ZTES ** 0.377C2 2.8E-4 * PINS ** 1.08
Mos Linear Ea 0.65 eVCl 0.01 4 0.00150 * TAH ** 0.488Pins 3.69 * GC5- ** 0.318(2 2,8E-4 * PINS ** 1.08iTransiLstor Gate Area 1349 * TRANS ** 0.609 (sq Ui)
Dielectric Thickn)es 4.93 / 'J•NS ** 0.286 (kA)
Bipolar Linear Ea 0.65 eVC1 0.01 4 0.00150 * TPI\NS ** 0.488Pins 8.69 CM-S ** 0.318C2 2.8E-4 * PINS ** 1.08
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The temperature activation energies were obtained directly from the tables
provided by the RA/AAT final report. The Cl factor equations were derived
by fitting the Cl factor data associated with the RA/AAT failure rate
models to an appropriate curve. The data and best fit curves are shown in
figure- 4-1, 4-2 and 4-3 for MOS digital, bipolar digital ai ] MOS and
bipolar linear ASIC/VHSIC microcircuits, respectively. The re itionships
between package pin count and circuit complexity for MOS digital, bipolar
digital and MOS and bipolar linear ASIC/VHSIC microcircuits are shown in
figures 4-4, 4-5 and 4-6, respectively. The data from which tbe
relationship betaeen total transistor gate area and circuit complexity was
derived Js shown in figure 4-7 for MOS digital and linear ASIC/VHSIC
mirrocircuits. The dielectric thickncss dependence on circuit complexity
for" MOS digital and linear ASIC/VHSIC microcircuits is shown in figure 4-8.
By applying the approach outlined in section 4.0, maximum junction
temperatures and maximum supply voltages were calculated for the four
AZCJkl ... tochrhologics as a function of circuit complexity1,. Figure•• s 4-9
and 4-10 show the junction temperature and supply voltage derating curves
for MOS digital microcircuits. Figures 4-11 and 4-12 show the junction
temperature and supply voltage derating curves for MOS linear
mu,-rocnrcuits. Figure 4-21 is also the junction temperature derating curve
for bipolar linear microcircuits. Since bipolar ASIC/VHSIC microcircuits
dc- not experience weiar out due to TDDB, supply voltage derating curves are
not calculated for the.se technologies. Fri.gure 4-13 shows the junction
temperature dcrutýi-g curves for bipolar digital microcircuits. The solid
lines on the grapls in each figure represent the best least squares fit to
the calculated denating values. These equat .ons of the lines are the new
stress derating criteria for each criti.calJity level.
35--
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Figure 4-1 C1 Factor for MOS Digital Microcircuitsl
I0
S"4--
00)
CCO0:)
e 000
C;C
CC t
00
3Z6
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Figure 4-2 CI Factor for Bipolar Digital Microcircuits 1
0 C3 U)C
- E U
• E
to
a)r
o C +
z 0
0"•- 0
a) I
E1
0 o
_ 0 q4 U 0
U, C)
37
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Figure 4-3 CI Factor for 140S and Bipolar Linear microcirc'Lits5
(D0C:-
C1CD
CO
z :
cc Ex
C:U
V 0
CI) q
0E 0
EECL00
C) 0
:3~
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Figure 4-4 Package Pin count for MOS Digital MiCrOcircultS5 7
00
0CLC
CD
4-'ý
cboD
0 " 03_C
z
T-1.
E0
o 0 0 0 0 0 0to) U') 4, C() j
39
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Figure 4-5 Package Pin Count for Bipolar Digital Microcircuits57
N E
> 0
(D 0)E 0_cc 0
0- 0CL0 QI C%
FLC CD
C oo o
0.0 0 0 0
(0 04
40
aee
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Figure 4-6 Package Pin Count for MOS and Bipolar Linear Microcircuits 5 7
0aLaCO
>0
o Eao ° 5°
EE
E x
,C_: 0 C0
0~0
"W~~ C04",
441
CO (
EZE
CI zn) & I CD,
00
00
ci41
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Figure 4-7 Tjransistor Gate Area for MOS Digital and Linear Microcircuit-s1
Ci)
0O
0 CoU) coc
O o 0
-IE EO
co EJ
co~
co f-c
~%~% 42
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Figure 4-8 Dielectric Thickm-ass for MO,,.. Digital and Linear Microcircuit-sl
Co-Co
C) 0
C c E
W (0)Z
C 0U
C:)
4Q ) >
- 0 CCo
ccCD
-CM
I-J
4-3
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Figur-e 4-9 Junction Temperature Derating for MOS Digital ASIC/VHSIC
L0
5cn ,*
,a) &-
.
0n(5o. 4-
C J CL C
E a 1 03 -
0)
LO~1 0" LO 0iO. 0) f-
44~oo
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Figure 4-10 Supply Voltage Derating for MOS Digital ASIC/VHSIC
CO,(Dp
>I
,)> I D
0.
C >
0 M
0 _ 45
o~k / .1
a5 >
< 45
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Figure 4-11 Junction Temperature Derat-ing forBipolar/MOS Linear ASIC/VHSIC
CI)!
o Lt
.o . _=__
1~. 1 a C 00
-- __- _" _0
':,tI I I~" 9 >
00
V __ __ ___oo
CO -5 _5 __
- ,,
CL l
,) 0 C0 0 L/
1I- 'IM
2
EE
CO O3 ocO u O U
-P w-- I - --E-
X4
~~CI I I I I I I I )I I I I
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iFigare, 4-12 Supply Voltage Derating for MOS Linear ASIC/VIUSIC
(D >
__ _ LO=
(1) 0
C/) J-1 I 50~o
N- (
I O~
0t
co t 0N (f) (T) )
47
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Figure 4-13 juny-tol- ¶Iemprerature Derating for Bipolar Digital ASIC/VHSIC
_____ ____LO
C, ~00
P CCj - -
EEM -0 E E
:L- E .
Z ili
C"
U) 0~ 0 0 U
0- It) (' 0 t- UI) 01J
48
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Supplementing the junction temperature and supply voltage derating
parameteas were the stress derating parameters outlined, by other derating
guideline sources and shown in tables 4-3, 4-4, 4-5 and 4-6 for MOS
digital, MOS linear, bipolar digital and bipolar linear microcircuits. In
keepirg with the general approach outlined in Section 3.0, and because of
the uncertainty of criticality assumed with guideline sources not
specifying three criticality levels, only those guideline sources supplying
derating criteria for three criticality levels were evaluated for inclusion
in the updated guidelines. For each parameter specified by these guideline
sources, a median value for the parameter was chosen. In the case where
the choice was between an even number of values, the average of the two
median values was calculated and then rounded up.. Priority was given to
those guidelines specifyirct advanced microcircuits, such as VLSI and gate
arrays. The remaining guideline sources were used only as a "sanity check"
of the updated stress derating criteria. Table 4-7 summarizes the new
stress derating criteria for ASIC/VHSIC microcircuits.
As addressed ii-, section 4.0, the complexity of the ASIC/VHSIC device is
limited by the criticality level. Although the higher criticality level
(Level I, for example) derating criteria allows a more complex device to be
used, the allowed stress is typically less than the strcss allowed at the
lower criticality level (Level II, for example).
For MOS ASIC/VIRSIC microcircuits, both maximum junction temperature and
maximum supply voltage are a function of circuit complexity. Therefore,
these two parameters can be conbirbad to form effective Safe Operating Areas
(SOAs) for these microcircuits. Figures 4-14, 4-15 and 4-16 display the
SOAs of MOS digital microcircuits for criticality levels I, II and. Ill,
respectively. In each graph, the top set of SOAs is for a ICWO gate
micocizrcuit the middle set of SoAs is for a 10,000 gate microcircuit and
the bottom set is for a 100,000 gate microcircuit. Multiple SOAs are
displayed as part of each set of SOAs according to the required lifetime of
the microcircuit. The "squareness" of the SOA indicates the level of
independence of the temperature and voltage factors.
49
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Table 4-3 ASICNHSIC MOS Digital Microcircuits Guidelines
DYNAMIC OUTPUT MAXIMUM MAXIMUM
CTF'-fUTY SUPPLY FREQU4ECY CURRENT JUNCTION OPERATINO
L.EVEL GUIDINE VOLTAGE (POMS) (FAN GUTI) TEMP, TEMP.
(PORy) Por" (dog C) (dog C)
AMB 70 80 8o as NL
C 75" 80 . 70(80) 85* NLI D 75* 80 70 (80) 85 * N1.
E 70' s0 80 as NILF 100 NL 80 NL 30 C FAL
A&B 85 80 85 100 NLC I0 t 8 0 7 5 ( 8 M) 0 0 N L ID so . 80 75 (80) 100 * N L.
E 80 8s 90 100 NLF 100 NL 90 NL 20 C FML
A&E a 90 90 110 NL
C 95 80 80 (90) 125 * NLI=. I i. * NI
E a 90 90 110 NLF 100 NL 100 NL 20 C FML
-- ~~~~ ~~ -___________ --- J-
0 90 9C 80 NL 85NIONE Hi- (Nomlnl - NL 80 110 NLSPECIFIED J NL 75 80 110 NI.
K 70* 80" 80* 95 NLL (NomInaJ) 70 80 100 NLM 8o NLI 80 125 NLW 100 50 80 65 PORV 30 C FML
X Voc +/-0,5V NL 75 125 NL
Kz-EY: FML - From Mexlmum UmIt- cw'zrpd'. M~~cc~iipoMS- PFiC6-i v-
NL - NW UglWd PORV - Percert of Rated Value
50
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Table 4-4 ASICNHSIC Bipolar Digital Microcircuits Guiaelines
DYNAMIC OUTPUT MAXIMUM MAXJMUM
rBITKALITY Qa.INE SUPPLY eMUPPY FREOUENCY CURRENT JUNCTION OPERATING
LEVaEL VOLTAGE VOLTAGE (POMB) (FAN OUT) TEMP. TEIP.(POFt) (pO" (Clog P (dw C')
A&B +/-3% NL 80 80 85 NL
C +/. 3%* NIL 75 * 70(70) * 55. NLD NL 75* 75 * 70 (70) * 85 NLE 4+-3% NL. I0 &0 85 NLF NL NL NL 70 NL 33' C FML
A&F3 +/-5% NL 90 85 100 NL
C +-5% NL 8go. 75(75) * 100 NL
D NL 80 o80 75 (75) * 100, NL
E +/-5% NL 90 90 100 NL
NL NL HL 80 NL 25 C MWL
C +/-5" NL 90* 80(80) - 125 * NL.D NL 85 90 E0 (80) 12L * NL
E Pe Sm. NL 05 90 1le; NL
F NL NL NL 900 NL 20 C FML
G +/-5% NL g0 80 NIL 85NONE H NL (Nonilna) NLi 80 110 4L.&P-CIFIOD J NL NL 75 so 110 NI.
K NIL 70 o80 801' 85 PIL
L NI. (NomInal) 70 100 NL
M 10 % NL NL 80 125 N',WNia '0 no POCiv 300FML
x +/-0.5V NL NL 75 12.- Ni.L
C~rt*xP~uaft P0MS Pmcwo of k Op~~x dMIoNIL U•o Dd POWN - PvrWOr of PW V
51
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Table 4-5 ASICNIVSIC MOS Linear Microcircuits Guidelines
C~nA-r UD- SUPI>tv INPUIT FRCO, OIUTPfT PO`NER MAX MAXCRI1CU~' OiIE~ VOLTAGE VOLTAGE (PM UFA-NT Gu) ISIP71N TEM OFP.
LEVL UES PORVO Form(PO (PON PTJ (dog C;) (dog C)
AMB 70 60 NL 70 NL so NLC 75' NL 80 * 70 (80) * NL 85. NLD 75' NL 80 * 70 (0)' NL a 1 N
E 060 NL 70 NL 80 NLF 060 NL NL 55 VP. ACFML
AMB s0o0 NL 75NL C5 NLBC 80* 70 ~ NL 75(80)' N 95' NL
O go' NL I 80' 75 (80)* NL 100* NLr 60 70 I NL so Nt. 95 NL
FM 70 0 NL NL 8 L 2 M
AC & 70' t 0 ) Nt. oin, Nt.
o 85* N. 80* so(w0) Nt. 125' NLF so 70 Nt. no Nt. 105 NL
Gi 90o 90 Nt. so 75 Nt. 95H- 80 s NL 70 Nt. 110 Nt.1~~If 70 70 7575 6o 110 NL
K so0. 100 Nt. SG 75"* 100 Nt.L (NomlnAi 75 Nt. 70 50 Nt. 125
MNt. 80 85 as 85 125 NLso8 65 s0 75 Nt. 6OPOfIV 30 C ML
L . 75_ 75 Nt. Nt. Nt 125 Nt.
"t.y C~xirAex Ma cutFML -From Maximrum Iimh
"'Worul cuea; w~gm v~r~tkw-s iiiýuqj 'P-' - Pemewi ol Maylmum Soect~eddfreodlng on da1vie type PORV/ - Parcerd ol Baled Value
Nt. - Nat LisWed
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Table 4-6 ASICNHSIC Bipolar Unear Microcircuits Guidelines
CRITICAJTY SUPPLY INPUT OUTPUT POWER MAXIMUM MAXIMUM
OUIDtEUIN VOLTAGE VOLTAGE FREQUENCY CURRENT DIS31PATION JUNCTION OPERATINOLEVEL (PORV) (PORM (POM8) (FAN OUl) (POTM TEMP. TEMP.
(PoI' (dog C) (dog C)
A&B 70 60 NL 70 NL 80 NL
C +/-3%' NL. 75' 70 (70) * NL 85 * NLD 75 NL 75• 70 (70) * NL 85 * NIL
E 70 60 NL 70 NL s0 NL
F 80 60 N1- NL 55 NL 30 C FML
A&i +5 70 NL 75 NL 95. NLh c5%0 70' NL 75(75)- NL 95 NL80' NL 80' 75(' NL 100 k
E 80 70 NL 80 NL 95 NLF 80 60 NL NL so NL 25 C FML
,&B 80 70 NL so IhL. 105 NL
C +/-5% 70 NL 80(80)- NL 105' NLD 85 NL 90 * 80 (80) NL 125' NLE s0 70 NL G0 NL 105 NL
80 60 NL NL 90 NL 20 C FML
NONE 8 50 70 NL 80 75 NL 85OPECIrF•ID H 75 80 NL "0 NL 110 NL
J 70 70 75 75 60 110 NLK g0o. 100 NL 80 75 100 NLL (Nominal) 75 NL 70 50 NL 125
M NL 80 85 85 85 125 NL
W so 65 so 75 NL 60 PORV 30 C FMILX 75 75 NL NI- NL 125 NL
"KEY' -C= t HAMwroudroLV PCFff Pwsr4w of fRmod VimNL - NW Uh' ** - Wormt cae; zlkght vwlatlons likotyFML - Fron MuYmRri I" depenrvIrhg on d" ce typePO.Me u Pwmw of Mamnrn uDidped
53
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Table 4-7 ASICNHSIC Stress Derating Criteria
-j r-- O ~ +
Lo
CS 6
-6 C 008,iO' n DnOU
Go ~ ~ ~ ~ 4 +ZC 0 1 t o ,c \ - r
C? 0
gE co 51111
:) . ?--~: c
.2, i , Z' -
-f 0
~~o~~Lo -*O~
c& ctd E LI w EcE 0 a) a
a 0 C >0 l-a
cn 2..L:E 54
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Figure 4-14 Criticality TLvel I SOA for MOS Digital ASIC/VHSIC
tLO
0"to 0
0
W 00
0
No -o 0o
q5 't 0
"-" o 00
S- -- - - -
0
C I Q)
400
0 C~0
CLC
- ~ r 0
0)j T) aD C-w " - f'
4- 0kg5
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Figure 4~5Criticality Level II SOA for MOS Digital ASIC/VHSIC
LO
00
LO0
0) 00
Uj) C 0o 0)
00
C4)0) > 0)
4.'40
0 I0oo 4) 04 0)c'
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Figure 4-16 Criticality I~evel III SQA for MOS Digital ASIC./VHS3ZC
LO1
LO
-L
0 40
u-) IT 0
0)0
C0 0:
C) -10
% _ s- 76 i
Co
4-1
'a MUC
>0n
4--
Cji co C
57
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4.2 MICROPROCESSOR MICROCIRCUITS
Tje stress derating criteria for microprocessors was developed similarly tothe ASIC/VHSIC microcircuits, with two exceptions. First, the lack of
stress-failure data and reliability models for bipolar or MOS linear
microprocessors precluded the development of derating criteria for thesetechnologies. Second, the circuit complexity factor, Cl, in the RA/AAT
failure rate model was a function of bit count. Therefore, stress deratingtables were generated for the three categories of microprocessors, 8-, 16-
and 32-bit, for both MOS digital and bipolar digital technologies. The
differences between the criteria in each table were the results of applying
the different device-specific attributes and stress-specific parameters tothe failure rate equation. These attributes and parameters included
temperature activation energy (PiT), circuit complexity (C1), number of
package pins (c2), total transistor gate area (LTDDDB) and dielectric
thickne-ss (LTDDB). The values or equations used in evaluating the
device/stress-specific attributes ar ouutlined in table 4-8z
Table 4-8 Microprocessor Device/Stress-Specific Attributes
Technology Attribute Value / Equation
SDigital_ Ea 0.35 eVCl 0.14C). 0.28cl 0.56Pins 11.07 * GAMES ** 0.342C2 2.8E-4 * PINS ** 1.08Transistor Gate Area 4047 * TRANS ** 0.463 (sq urn)Dielectric Thickness 28.18 / TRXIS ** 0.412 (kA)
Bipolar Digital Ea 0.60 e7Cl 0.06C1 o0.12C1 0.24Pins 9.16 * GATES ** 0.377C2 2.8E-4 * PINS ** 1.08
58
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The temperature activation energies and C1 factor values were obtained
directly from the tables provided by the RA/AAT final report- The
relationships between pin count and circuit complexity for MOS digital and
bipolar digital microprocessors are the same as the relationships
associated with MOS digital and bipolar digital ASIC/VHSIC microcircuits,
respectively. The. circuit complexity dependence of total transistor gate
area and dielectric thickness for MOS digital microprocessors are shown in
figures 4-17 and 4-18, respectively.
By applying the approach outlined in Section 4.0, maximum junction
temperatures and maximum supply voltages (MOS) were calculated for the two
microprocessor technologies, three bit counts each, as a function of
circuit complexity. Figures 4-19 and 4-20, figures 4-21 and 4-22 and
figures 4-23 and 4-24 are the junction temperature and supply voltage
derating curves for MOS digital microprocessors of 8-, 16- and 32-bit
complexities, respectively. Figures 4-25, 4-26 and 4-27 are the junction
temperature derating curves for 8-, 16- and 32-bit bipolar digital
microprocessors, respectively. The solid lines on the graphs in each
figure represent the best least squares fit to the calculated derating
values. These equations of the lines are the new stress derating criteria
for each criticality level.
It is noted here that a review of the range of complexities within each
category of microurocessor showed the transistor counts varied marginally
for 8-bit microprocessors (22,000 to 27,000 transistors) as compared to
16-bit (30,000 to 120,000 transistors) and 32-bit (80,000 to 1,000,000
tmasistorsj) wicroprocessors. Therefore, an approximate worst case 8-bit
microprocessor complexity of 10,000 gates was assumed and the stress
derating equations for 8-bit microprocessors were changed to the values of
those equations at the 10,000 gate complexity.
supplementing the junction temperature and supply voltage deraUlng
parameters were the stress derating parameters outlined by other derating
guideline sources as shown in tables 4-9 and 4-10 for MOS digitEI
59
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microprocessors and bipolar digital microprocessors, respectively. In
keeping with the general approach outlined in Section 3.0, and because of
the uncertainty of criticality assumed with guideline souirces not
specifying three criticality levels, the method for evaluating tlhe stress
derating criteria for microprocessors was the same as the method used forevaluating the stress derating criteria for ASIC/VHSIC microcircuits.
Table 4-13 summarizes thc nmw stress derating criteria for microprocessors.
60
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Figt--e 4-?- Transistor Gate Area for MOS Digital MicroprocessorsI
CO)
0C I) ( D_ - _ _ _
0E E
,Q. :3 m O.
0 E
L---
0 OI
-2- r)
41!1
COC
(~ 61
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Figure 4-18 Dielectric Thickness for MOS Digital Microprocessors 1
LO
(IIN
00
I - _ _ CXE
C)0 <0O
0 0
00w Eo
00
< Q
-C X
62')
CO.?)
o L~ C C) K1C
62
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Figure 4-19 Junction Temperature Derating for8-Bit MOS Digital Microprocessors
LC4)
0 1 tE" Cr
09.•-
/: 00 :.: 4 . ",• '• m •-
CL -- O
,• ---
nD-,-
to 0- U1. 0 • O Cit) C* r_ U*
63 :----
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Figure 4-20 Suppl~y Voltage. Derating for
8-Bit MOS Digital microprocessors
W(a
CLz CL 0 :3 -
00
E'tE 7
C)e
tO C' O ) CV)IL 1j a ( f
64
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Figure 4-21 Junction Temperature Deratingfor 16-Bit MOS Digital microprocessors
_____CD
I _ _
0-•0
U) I- - _ L6
o /(1
C)A
€-,
CO LO OC'-2•D 00 )
265
:3 CD
Z. E- / -
CI) LLJ
00
CII
Q 0 ) 0 tf '
65
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Figure 4-22 Supply Voltage Derating
for 16-Bit MOS Digital Microprocessors
(0
0 0 ECO>
CC)> 0.L- Ci >!CL) CIEX
00
,O 0"-_ I /E 0"E
.-- E 0)0
- - - -
- U
>>
V)6>
0C X' ) (0 C
0 Y.1
66
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Figure 4-23 Junction Temperature Deratingfor 32-Bit MOS Digital Microprocessors
I G)
/ "-
CO
0 E0 x
0 0-
0 >'
•4- CO-J "
0CzC
U- 0 tno •o 0 n o '
67 ---
l'o
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Figure 4-24 Supply Voltage Derating
for 32-Bit MOS Digital Microprocessors
* >
0U
co0)
q >
':1) / 0 --
C)L IQ
00
E 0)
._ -
0 I I
0i) >
) Li)
4O >
00
C9 L
co Li) C' ) (0 C C)
68
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Figure 4-25 Junction Temperature Deratingfor 8-Bit Bipolar Digital Microprocessors
, U)
o,
SE D0 0
.=
.0 ~4) 4)I>-j
S' ' 4-J 0
00
00. 0
LLC
LO 0 U") 0 to 0 LO0I'- U-) (i 0 I1- U) 04
69
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Figure 4-26 Junction Temperature Deratifl(
for 16-Bit Bipolar Digital Mi~croprocessors
7F)4)
0 U-)0(.3E >x
(D0
4) 0
OI1 a --
0.2 '
C) 0
EE
E C
07
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Figure 4-27 Junction Temperature Deratingfor 32-Bit Bipolar Digital Microprocessors
I 'E -
>
I 0"
0.)So., g, =.
S__ /I"E I
0L-CL E _ __- LO
O InOI 0 In 0f(-- U' C4 0 0- In 04
7)1J
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Table 4-9 MOS Microprocessor Guidelines
DYNAMIC OUTPIT MA)OMUM MAXIMUMCUmNCAUTY SUPPLY FFEOUENCY CURRENT JUNCTION OPERATING
LEVEL GUIOEUNE VOLTAGE (POMS) (FAN OUT) TEMP. TEMP.T (OV (POW (deo C) (dog C)
A&B 70 80 80 85 NLC 75 * 80 * 70 (80)* 85 NLD 75 * 80 * 70(80)- 85* NLE 70 80 80 85 NLF 100 NL 80 NL 30 C FML
A&B 85 80 85 100 NLC 804 80 * 75 (80) * 100 * NLD 80* 80 * 75 (80) * 100 * NLE 80 80 90 100 NLF 100 NL 90 NL 20 C FML
AD5 90 90 110 NL
C 85 80* 80 (90) * 125 * NLD 85* 80 80(90) * 125 * NL
E 80 90 90 110 NLF 100 NL 100 NL 20 C FML
G NL 90 NL NL 85NONE H (Nominal) NL 80 110 NLSP..iFIED J NL 75 80 110 NL
K 70* 80* 80* 85 * NLL (Nominti) 70 80 100 NLM 80 NL 80 125 NLW 100 50 80 65 PORV 30 C FMLx Vcc +/-0,5V NL 75 125 NL
KCY: FML - From Maimum Umit* - Comp4ex Mlro•irCulRN POMS - Po.rcet of Makimum SpecifledNL - Not Ustod PORV - Pero*M of Rated Vaiue
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Table 4-10 Bipolar Microprocessor Guidelines
FDCED DYNAMIC OUTPUT MAXIMUM MAXMUM
CI TICALITY GUIDEUNE SUPPLY SUPPLY FRFQUENCY CURFENT .JUNCTION OPERATING
I.EVE. VOLTAGE VOLTAGE (POMI (FAN OUT) TEMP, TEMP.
(PORV) (PORV) (dg C) (do C)
A&B +/-3% NL 80 8O 85 NL
C +/- 3% NL 75. 70 (70) * 85* NL
o NL 75 75* 70 (70) * 85* NI.
E +/-3% NL so 80 85 NL
F NL NL NL 70 NL 30 C FML
A&B +1-5% NL 90 85 100 NL
C +/-5%* NL 80* 75 (75) * 100 * NL
D NI. 80 80 75 k75) * 100 * NL
E +/-5% NL 90 90 100 NL
F NL NL Ni, 80 NL 25 C FML
A&B +/-S% NL 95 j 90 110 NLC 5% NL o s 80(80) * 125 * NL
D NL 85* 90 *U(&i 125 * NL
E Per Spec. NL 95 90 115 NL
F NL NL NL 90 NL 20 C FML
O +/-5% NL 90 NL NL 85NONE H NL (Nominal) NL 80 110 NL
SPECIFIED J NL NL 75 80 110 NL
K NL 70* 80 s0 85 * NLL NL (Nominal 70 80 100 NL
M 10% NL NL 80 125 NL
W +/-5% NL so so 65 PORV 30 C FML
X 0.5v NIL NL 75 125 NL
KFY: FML - From MlajmUrr
" Cmwiea mkro¢ POMS : P•ort of MagIJvrn Sokd
NL - NoI Ujgd PORV PWVV0 Of PAW Vmkm
73
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Table 4-11 Microprocessor Stress Derating Criteria
66,,
CO O
= oo - •
CO (D ~l-
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+
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74
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4.3 PROM MICROCIPCUITS
The. stres derating criteria for PROM devices was developed similarly to
ASIC/VUSIC miarncircuits, with exceptions for EEPROMY. These exceptions
centered (in the need to include the LCyC term in the failure rate model
of eqwittion (2). The differences between the criteria in each table were
the results of applying the different device-specific attributes and
stress-specitl parameters to the failure rate equation. These attributes
and parameters included temperature activation energy (PiT), circuit
complexity (C3), number of package pins (C2), total transistor gate area
(1 TDDB) and dielectric thickness "LTDDB). The values or equations used
in evaluating the device-spacific and stress-specific attributes are
outlined in table 4-12.
The temperature activati.on energies were obtained from the pre--release
version of MNIl-HDBK-217 Revision F. The Cl factor equations were derived
by fitting the Cl factor data associated with the RA/AAT reliability models
to an appropriate c,,rve. The CI data and best fit carves are shown in
figures 4-28 anid 4-29 for MOS PROMS and bipolar PROMs, respectively. The
value for maximum pin count was derived by exarniation of current supplier
Table 4-12 PROM Device/Stress-Specific_ Attributes
___~ahn AtrhE ciuationI7iirr I - _ aIi _-- _
WIG Ea 0.60 evC! 0.00085-: 5A5E-6 * Bfl5 w* 0.515Pins 40C2 2.88E-4 * PINS ** 1.08Tr-ansistor Gate Area 3..209E6 (sc urn)F1)ic1c--ric thickness 2.31 / BITS ** 0. 175 (VA)
BiroAlar Ea 0. 60 cVCl 0.0094 4 6.20E-5 * BITSJ *k 0.514PinEs 40(22 2-8E-4 * P1715 ** 1.08
"¶5
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Figure 4-28 Cl Factor for MOS PROMS 1
I LL
OO 0
4* C Eto E0~
f-r x
LU .
I E El
c'z
C- 04)
o7 6
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F.'gure 4-29 C1 Factor for Bipolar PROMsI
LL
-- I - (0--
U +
001 m -
0 C0
SE 0
0. c E
00
i9 i t.._o Ir
ca
4-
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0 =
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data books which described memory complexities up to one megabit- The.
total transistor gate area for MOS PROMs was extracted directly from the
RA/AAT final report. The dielectric thickness dependence on memory
complexity for MOS PROMs is shown in figure 4-30.
By applying the approach outlined in section 4.0, maximum junction
temperatures and maximum supply voltages were calculated for the two PROM
technologies as a function of memory complexity. Figures 4-31 and 4-32
show the supply voltage derating curves for MOS PROMs excluding EEPPh)Ms and
EEPROMs, respectively. The maximum supply voltage for EEPROMs is lower
than the maximum supply voltage for other PROMs because it was. traded off
with the number of write cycles. It is noted, however, that the difference
in supply voltage between EEPROMs and other types of PROMs of similar
complexity is at most 0.85 volts. In the trade-off between supply voltage
and number of write cycles for EEPROMs, the only guideline used was the
requirement was that the supply voltage remain above 5V for all EEPROMs up
to"' 1 Mbit complexity for any criticality level. Figure 4-33 shows the
write cycle derating curves generated for EEPROMs. Since bipolar PROMs do
not experience wear out due to TDDB, supply voltage derating curves are not
calculated for this technology. The solid lines on the graphs in each
figure represent the best least squares fit to the calculated derating
values
Supplementing the junction temperature and "*-"7s ,VltAe derating
parameters were the_ slress derating parameters outlined by other derating
guideline sources as shown in ta•bes 4-13 and 4-14 for MOS PROM devices and
bipolar PROM devices, respectively. In keeping with the general approach
outlined in Section 3.0, and because of the uncertainty of criticality
assumed with guideline sources not specifying thiree criticality levels,
only those guideline sources supplying derating criteria for three
criticality levels were evaluated for inclusion in the updated guidelines.
For each parameter specified by these guideline sources, a median value for
the parameter was chosen. In the case where the choice was between an even
78
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Figure 4-30 D~ielectric Th~ickness for NOS PROMs 1
IF
0 0
tO E
Tc_ __ _ _
____ ___-I-. -_________ L OCD ~ C -W.
2 L.
~U 0~; ------ 6
OR(C)C 6L79
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Figure 4-31 Supply Voltage Der-athig for MOS PROMs Excluding EEPROMs
I-
!! ')I ,D
00
CmD
080
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z >
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Wa f
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Figure 4-32 Supply Voltage Derating for EEPROMs
U'))ix
-l
I• -II
U) - - --- - . O-
CL
/ /--
/ //0I I l
_'I- -
I _//__-IL)_
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Figure 4-33 Write Cycle Derating for EEPROMs
LO
(D i
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x
Cu z
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08 -. ... LO Lo73o o o
0 0n 0 0n 0 0 0
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Table 4-13 MOS PROM Guidelines
DYNAMIC OUTPUT MAX]MUM MAXIMUM
CmCAUTY SUPPLY IREOUENCY CURRENT JUNCTION OPERATING
LEVEL GUIDENE VOLTAGE (POMS) (POTEMP. TEMP.(PORV) (deg C) (deg C)
AB70 80 80 85 NLC 75* NIL 70 * 85 * NILD 75* NIL 70 * 85 * NLE 70 80 80 85 NLF 100 NL 80 NL 30 C FML
A&B 85 80 85 100 NILC 80 * NIL 75 * 100 * NILo 80 * NIL 75 * 100 * NLE 80 80 90 100 NLF 100 NL 90 NL 20 C FML
A&B 85S 90 -90 11!0 Nt"
C 85* NL 80* 125* NLD 85* NL 80 * 125 * NLE 80 90 90 110 Nl-F 100 NLt 100 NL 20 C FML
SG NL 90 NL NL 85H (Nominal) Nt 80 110 NtLC Nt 75 80 110 NtL
K 70* 80* 80* 85* NLL (Nominal) 70 NtL 100 NLM 80 NL 80 125 NLW 100 50 80 65 PORV 30CFM.LY Vc? +/-0.SV NL 75 125 NL
KEY: FML . From MuNJnumn Umlt* - Complex Microcircuit POMS - Per.MTat 01 Mxmmurn Spncffie
NL - Not UiW PORV -' Pw.tt of Ratad VaAke
83
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Table 4-14 Bipolar Prom Guidelines
FIOED DYNAMIC OU'FUT MAXIMUM MAIMUM
CP,;TFALITY GUIDELUNE SUPPLY SUPPLY FREQUENCY CURRENT JUNCTION OPERATING
LEVEL. VOLTAGE VOLTAGE (POMS) (PORW) TEMP. TEMP.
NI.NI-- 70NI(PORV) (dog C) ((*a C',
A&B +/-3% NL so so 85 NL.C +/- 3% NL NL 70 * 45 . NL i ,=
ID NL 75 *NL 70 * g5 * NL E
E +1-3% NL 80 so 85 NLF NL NL NL 70 NL 30 C FML
A&B +/-5% NL go as 100 NLC -5% *NL NL 75 * 100 * NLD NL. 80 *NL 75 * 100 *= NL
E +/-5% NL 90 90 100 NLF NL NL NL so NL 25 C FML
MEB ,.-,% NL 95 90 110 NLC /-5%* NL NL 80s 125 * NLD NL 85* NL 80* 125 * NLE Per Sp•c. NL 95 90 115 NLF r4L NLL so NL P0 C FMIL
NONE G +/-5% NL 90 NL NL 85SPEOFIED H NL (Nominal) NL 80 110 NL
J NL NL 75 80 110 NLK NL 70* 80 80. 85 . NLL NL (Nomlnal) 70 NL 100 NL
M 10% NL NL 80 125 NL.W +/-5% NL 5s 80 65 PORV 30 C FML.X +/- 0.5V NL NL. 75 125 NI J
KEY: FML * From Mrun LmUA. . Canipin kx ocVcift POMS" Pow"~ of Madmu¶ SpeogodHL W Mof LAWd PORV - Pvot of 'Nhd Van
84
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number of values, the average of the two middle values was calculated.
Priority was given to those guidelines specifying advanced microcircuits,
such as VLSI and gate arrays. The remaining guideline sources were used as
a "sanity check" of the updated stress derating criteria. Table 4-15
summarizes the new stress derating criteria for PROM microcircuits,
including the pertinent stress derating criteria from the current version
of the Guidelines.
8,!a)
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Table 4-15 PROM Stre~ss DeratiJ-fg Criteria
CC
01 cL C L^ . m W%~ Cu.ca 00C"J ~ ~ O(J
o 81 *- eaion
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ao 4--.
p~ 46
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-6 -1:sIu t LI L
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:>:- >~~~3L >> U4.U 4 40C
L)I. 31 d 3
>,>~ 9 --. 04 86
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4.4 MICROCIRCUIT APPLICATION NOTES
The following application notes for advanced technology microcircuits were
developed from a review of applicable literature, supplier surveys andother stress derating guidelines. These application notes may also be
found in Appendix A.
Digital Microcircuits:
1. Advanced technology microcircuits are sensitive to ESD.2. Unused inputs should be connected to a supply voltage or grcand.3. Supply filtering is required to filter out transients.4. Heat sinks may be required to maintain der;ted junction temperatures.5. Design margJns should be used for input le-akage (+100%), fanout (-20%)
d frequency (-10%).6. uood engineering judgement should be used to derate other microcircuit
characteristics, including hold and propagation delay times, toproduce a conservative design.
7. circuit design must avoid application of reverse voltages on deviceleads.
8. Do not exceed the current density derating described by the equationCurrent Density = 366 / (Temperature in deg. C ** 1.67)
or 5E5 A/cm2 , whichever is smaller, for aluminum-based metallizedmcrocircuits for either internal circuit operation or output driveroperation (see figure 4-34).
9. (Bipolar) Supply voltage deviations from rthe specified nominal willshift. internal bias points which, when coupled with thermal effectscan cause erratic performance.
10. (MOS) Input destruction may cxxur by shorting leads during assembly.11. (MOS) High speed transients may result in parasitic bipolar latch-up.
Linear Microcircuits:
I. Each liiear device is unique and the designer should have a thoroughknowledge of its application requirements to assure that the device isoperated within its performance envelope at all times.
2. Heat sinks may be required to maintain derated junction temperatures.3. Design margins should be used for gain (-20%) and offset voltages and
currents (+50%).4. The circuit design must avoid application of reverse voltage on device
leads.5. Do not exceed the current density de- ating described by the equation
Current Density = 366 / (Temperature in deg. C ** 1.67)or 5E5 A/cm2, whichever is smaller, for aluminum-based metallizedmicrocircuits for either internal circuit operation or output driveroperation (see figure 4-34).
87
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Figue 434 a~cu~mcurrent tXonsitY fýor ImircrociXcuits
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5.0 MIMIC DERATING GUIDELINES
For advanced technology MIMIC devices, the RA/AAT reliability modelsI can
be summarized in general form by
I = PiQ * [(CIA * Pi.TA + ClP * PiT) * PiA + C2 * PiE) * PiL (3)
where:
L is the MIMIC failure rate in failures per million hours,
PiQ is the quality factor,PiTA is the temperature acceleration factor for active devices,
PiTP is the temperature acceleration factor for passive devices,
PiA is tho MIMTC application factor,
PiE is the application environment factor
PiL is the learning factor,
CIA is the circuit complexity failure rate for active devices, in
failures per million hours,
CiP is the circuit complexity failure rate for passive devices, in
C2 is the package complexity failure rate in failures per million
hours.
A review of the literatureI01-122 concerned with MIMIC failure, during
the time since the RA/AAT failure rate models were generated, resulted in
no change to this basic model.
The stress parameters and attributes that directly affect the calculated
failure rate for a MIMIC devict: are embedded in the Pj and complexity
failure rate factors of the reliability model. To extract the maximum
stresses allowed for each criticality level from the factors in the
reliability model, L in equation (3) must be set to the maximum failure
rate allowed by each criticality level. Since MIMIC devices were not
included in either the current version of the Guidelines or any version of
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MIL-IliIBK-217, txiese maximum failure rate-s are not specified in table 3-3.
Therefore, an alternate approach was used to bound the failure rate tor
each criticality level. It was noted that the maximum failure ratescalculated for silicon microcircuits closely approximated the failure rates
that would Ze calculated given probabilities of success oZ 0.9990, 0.9900
and 0.9000 at 10,000 hours for criticality levels I, II and III,
respectively. The actual failure rates associated with these threeprobabilities of success are 0.1001, 1.0050 and 10.5361, respectively.
These three failure rates were Lised in the apprcach for developing stress
derating criter-ia in a fashion similar to the approach used for advanced
technology silicon microcircuits. The parameters and attributes of the
failure rate model z ctors were separated into three groups, one group for
criticality-specific (CS) attributes, one grotl.p for device-specific (DS)
attributes and the other group for stress-specific (SS) parameters. Table
5-1 outlines the relationship between the factors in the failure rate
equation and the distinction between criticality-specific, device specific
ana stresis-specific parameters and attributes associatecd with tne tactIs,
There were two types of device-specific attributes, technology and
complexity. The technology attribute of the C2 factor was handled by
noting that the pin count for most MIMICs does not exceed 10 pins. The
packaging technology selected was the one that gave the highest failure
rate for a 10 pin package according to th. RA/AAT final report. Having
boLud tU= package t . ,com ti_ •h cuit complexity attribute was handled
by noting that the relative difference in values of the CIP factors Zor
MIMIC devices with 11 to 100 passive elements and MIMIC devices with
greater than 100 passive elements was less than 30 percent, and that many
MIMIC devices had more than. 10 passive eLements. Therefore, the CIP factor
for Ai4MICs with greater than 100 passive elements was used to represent the
CIP factor for MIVICs with 11 to 100 passive elements. Four sets ofderating criteria were developed t. handle the tvio CIA and two (iP circuit
complexity categories of MIMIC devices.
90
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Table 5-1 Attributes and Parameters of MIMIC Model Factors
Factor Type Attribute / Parameter
PiQ CS Application Environment
PiTA SS Channel Tmzen ature
PiTP SS Ciannel Temperature
PiA N/A Applicaticn
PiE C Application Environment
PiL CS Years In Prcdadtion
CIA IS Circuit COmplexity, Active Devices
CiP DS Circuit Omplexity, Passive Devices
C2 MS Pacuage Tenology
The criticality-specific attributes included application environment and
years-in-production. The application environments for the PiQ factor were
S-Level, B-Level and B-Level for criticality levels I, II and III,
respectively. The application environments for the PiE factor were SF "
Au and GF for criticality levels I, . and III: respectively. These
application environments were chosen since thc y were the most closely
related to the application environments outlined in the current version of
the Guidelines. The years-in-production attribute for the experience
factor, PiL4 were 2 years, 1 year and 0.75 years for criticality levels I,
II and ]II, respectively. These years in production were chosen based upon
current experience with component procurement. for systems that can be
categorized by the definitions given for each criticality level.
9"
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The stresss-srp2f c parameters, as mentioned previously, a~e the only ones
that, when changed, result in a different failure rate for any given
MIMIC. The channel temperature parameter was the only parameter that could
be varied to obtain the maximum failure rate for the MIMIC. With the
device-specific, criticality-specific and stress-spescific attributes and
parameters defined, the maximum cbannel temperature derating criteria was
developed.
The criteria in the MIMIC stress derating table was the result of applying
the device-specific attributes and st'uss-specific parameters to the
failure rate equation. These attrijhtes and parameters included
temperature activation enezgy (PiTA and PiTP), circuit complexity (CIA and
CeF) and number of package pins (C2). Table 5-2 outlir.es the values used
in evaluating these device/stress-spec.fiu attributes.
'Ihe dependemo of failure rate and proL,!cility of success at 10,000 hovrs
of o;pcrticn are shown in figures 5-1 5 •-2, respectively. by applying
the approach outlined in sections '1.0 and 4.0, the maximum channel
tenperature is calculated by setting Uc KIMIC failure rate of equation (3)
to the failure rates of the three criticality levels. The channel
temperature derating criteria for .. IC devices is found in table 5-3.
Table 5-2 MIMIC De-vicertresii-Specific Attributes
Technology Attribute Value / Equation
GaAs Ea (Active) 1.50 eVEa (Passive) 0.43 eVClA 7.22UIP 2.94pins 10C2 2.8E-4 * P2IS ** 1.08
92
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Figure 5-1 MIMIC Failure Rate
LO
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El4 c
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Figure 5-2 MIMIC Protmability of 2uccess at 10,000 Hours
00
tom
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oc 6oý 6 '1 6 p0 C 0C
94
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Table 5-3 MIMIC Stress Deratirig Criteria
"000 u uj
4,
0
~ VUAV A A
a.~L uJa.m
C. a.
'~ 95
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It is noted here that the calculated derated channel temperature stress for
level IiY mission criticality (approximately 160 to 165 deg C) was above
the region of validity of the RA/AAT reliability model. Therefore, the
maximum channel temperature for level III criticality was set to the
maximum valid channel temperature of 150 deg C.
Since existing stress derating guidelines have purposely affected the
observed failure rates of components used in applications corresponding to
one of the three criticality levels, it was necessary to review the
existing stress derating guidelines to determine their relevance in being
inlluded in the updated stress derating guidelines, given that the factors
being derated were not explicitly included in the current failure ratemodels. It was determined that none of the identified fourteen guideline
sources pr ovided MIMIC stress derating criteria. Therefore, the updated
stress derating criteria for MIMICs is limited to only the newly created
criteria based upon the updated RA/AAT reliability models.
MIMIC APPLICATION NOTES
The following application notes for MIMIC devices were developed from a
review of applicable literature, supplier surveys and other stress derating
guidelines. These application notes may also be found in Appendix A.
1. The enviromrent of the internal package cavity of the MIMIC must bekept inert.
2. Precautions must be observed during electrical test to preventpotential latent failure due to overstress.
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6.0 POWER TRANSISTOR DEMAT GUIDELINES
Power transistors are designed for power anplification and harndling high
voltages and large currents. The main concern with power transistors is
the high absolute values of power and the limitation of operation iuposed
by second breakxown.
Stress derating guidelines were generated for three classes of power
transistors, silicon bipolar, GaAs -nd MOSFET. For silicon bipolar power
transistors, an approach similar to the microcircuit atproach %was used to
develop the stress derating criteria. For GaAs powr MESFETs, adequate
data was accumulated which allowed the generation of a temperature
dependent failure rate mciel. For power MlSFETs, it was determnied that
the currently accepted derating policies were adequate in providing the
margins of safety and sucoess needed in the intended applications. Reviews
of the literature123- 1 5 9 , supplier surveys and available stress derating
guidelines from governmnt and iniustnr sou•ces were used to evaluate and
urpate the stress derating criteria for these types of power transistors.
The application notes for power transistors were also developed froa a
review of applicable literature, supplier surveys and other stress derating
guide-lines. These application notes may be found at the end of this power
transistor section and in Appendix A.
6.1 SIL103• O kLFIAR POWEIER MANISIORS
The junction teap..xture, Tj, in a silicon bipolar power transistor
increases a., thc the x increases. The maximum value of T! is limited
by the tekv-ature a" which the base region of the transistor becX1Is
intrinsic, that is, the collector is effectively shorted to the emitter and
transistor actio.i o ases. 'The tenperature and power handling ability of a
trdnsistor can be inproved by providing adequate heat sink for efficient
thermal dissipation, providing a large enough emitter stripe width to
97
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reduce orent density and preferring low voltage, high curre-nt application
to high voltage, low currtnt applicatiom,. Tfe latter oondition results in
higher tenrature rises at the stripe centers. Consequently, both power
and junction teq arature stresses need to be derated.
The use of power transistors is often limited by a phencumvo called second
breakdown, wViich is marked by an abnupt decrease in dek•vice voltage with a
siavltareous intenval ccsstriction of current. For high pFer devices,
operation zust be confined to a safe operating area (SOA) so that permaz nt
damage caused by the second br•-kdocn can be avoided, Figure 6-1 shows a
typical SCA for a silicon power transistor oqei-ated in the cxmon-euAitter
configuration. At the upper left (A), collector load lines are limited by
current-carrying ability. The DC thermal limit (B) is determined from the
thermal restanoe RtI of the. device,
Rth = (Tj - To) / P (4)
where P is the power dissipated. Therefore, the thermal limit defines the
maxinum allowed junction tenperature, where
Rth(peak) = (Tj (max) - TO) / (IC x VCE) limit (5)
If Tj (max) and Pth~peak) are assumed constant, then
(IC X VCE) limit = (Tj (max) - TO) / Rth(peak) = comntant. (6)
Thus a straight. line relationship with slope=l exists h ..n Ln(Ic) and
In (VCE). At higher voltages and lower currents, the temperature rise at
the stripe center is responsible for tLe secoml breakdown, and the slope
(C) is generally between -1.5 and -2. The device is eventually limited by
the first breakdoW voltage, or avalanche, in the SOA as indicated by thle
verticai line (D). For vmperatures higher than To, the SOA is reduced.
All portions of the SQA should be derated to provide margins of safety as
needed for application.
98
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Figure 6-1 Typical Power Transistor SOA
aO
aQ-0
0~ C)
0
OL
0/ - -
C)) o
"o 0
CC;
o' I . / •_•°_,
- -
I-9
1 • -
!~ 0
C.,.r'-
99 '
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For silicon bipolar power transistors, the MIfj-IU)B!<-217E Notice 1
reliability mod-11 6 9 has the form
L = Lb * PiA * PiR * PiS * PiQ * PiE * PiT (7)
uhere:
L is the transistor failure rate in failures per million hours,
Lb is the base failure rate,
PiA is the application factor,
PiR is the power rating factor,
PiS is the voltage stress factor,
PiQ is the quality factor
PiE is the application environment factor, and
PiT is the tperature acx-relration factor.
A 'reVi.e of the literatuvre oo_.exvrnd with silicon bipolar power transistor
failure, during the tine since 'Lr-HDBK-217E Notice 1 failure rate models
were gene-rated, resulted in no dcange to this basic model.
The stz3!ss parameters and attributes that directly affect the calculated
failure rate for a silicon bipolar power transistor are embedded in the P!
factors of the reliability model. To extract the maxiiuam stresses allowed
for each criticality level fron the factors in the reliability model, L in
equation (7) must be set to the maxi.mu failure rate alimmd by eachcriticality level. These maxinum failure rates arm specified in table
3-j. In the approach to develop stress derating criteria for silicon
bipolar power transistors, the parameters and attributes of the failure
rate L=Idel factors were separated into three groups, one gruup for
criticality-specific (CS) attrilbutes, one group for device-specific (DS)
attributes and the other group for stress-specific (SS) parameters. Table
6-1 outlines the relationship between the factors in the failure rate
equation and the distinction between criticality-specific, device-specific
and stress-specific parameters and attrbiutes associated with the factors.
100
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Table 6-1 Attributes and Pa-_-ameters of Silicon Bipolar Powe:
TransLitor Model Factors
Factor Type Attribute / Parameter
Lb N/A Base Failure Rate (constant)
PiQ CS Application Envirornrnt
PiT SS Junctiorn Tet-erature
PiE CS Application Dnv:-xrm4nt
PiA N/A Application (cnintstant)
PiR SS Power Rating
Pis SS Voltage Stress
In tnis power transistor reliability model, tilere were no device-specitic
attributes. The only criticality-specific attribute was the application
environment attribute. The application environments for the PiQ factor
were JANTXV, JANTX and JAN for criticality levels I, II and III,
rec-ptive:.y. The application environments for the PiE factor were SF,
AUF and ir for criticality levels I, II and III, respectively. These
application environments ware chosen since they were the most closely
zelated to the application environments outlbied by the criticality levels
in the current version of the Guidelines and resulted in the highest
failure rate for the criticality level they represented.
The stress-specific parameters, as mentioned previously, are the only ones
that, when changed, result in a different Lailure rate for the given power
transistr. These parameters, junction temperature, breakdown voltage and
power rating, are the ones that can be traded-off to obtain a failure rate
similar ro the maximum failure rate that was calculated using MIL-HDBK-217D
Notice 1. As shown in table 6-2, the stress specific attributes include
temperature activation energy (PiT) and voltage acceleration (PiS).
101
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/Table 6-2 Silicon Bipolar Power Trcansistor
Stress-Specific Attributes
Technololycx Attribite Value / Equation-
Silicon Bipolar Ea 0.18 eVPiS 0.045 * exp [3.1 * A/R]
The approach taken to develop the bounds for these stress-specific
parameters first assumed the power rating was the same as the power rating
used to develop the maximum failure rate (200 W). Then, the derating of
the remaining stress-specific parameters associated with the other
reliability model factors, namely breakdown voltage and junction
temperature, were equally weighted in calculating a similar failure rate.
The equal weighting o: the stress p-raiametjers rcz,1•.•d in derating both
voltage and temperaturi.e to 65%, 85% and 90% of their maximum ratings for
criticality levels I, II and III, respectively. Since the conservative
maximum rating for silicon bipolar power transistors is 150 deg C, the
junction temperature derating for criticality levels I, II and III are 95
deg C, 125 deg C and 135 deg C, respect.vely.
Supn eknnting the breakdown voltage and junction temperature derating
parameters were the stress derating parameters outlined by other deratingguideline sources shown in table 6-3. In keeping with the general approach
outlined in Section 3.0, and because of the uncertainty of criticality
assumed with guideline sources not specifying three -,riticality levels,
only those guideline sources supplying derating criteria for three
criticality levels were evaluated for inclusion in the updated guidelin~es.
The" - aining guideline sources were used only as a "sanity check" of that
updated stress derating criteria. Table 6-4 summarizes the new stress
derating criteria for bipolar silicon power transistors.
102
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Table 6-3 Silicon Bipolar Power Transistor Guidelines
MAXIMUM SAFE S• ONOF
MPOWER SFWE BREAKDOWN ON-OFF
JUNCTION POWER OPERATIN43 OPERATING VOLTAGE TEMPERATUREJUTC GUIDELNE T TEMPCIR E OSSIPAT'ON AREA AREA (PORV) CYCLES
EM (POR V) (POw, Vc0 (POFr), IC
A&B 95 50 70 Vce 60 IC 60 NLC 95 50 70 Vce 60 Ic NL. NL
0 NL NL NL NL NL NL
E (55 PORV) 50 70 Vce 60 Ic 60 Fig. 6-4
F (55 PORV) 55 55 Vce 55 Ic 60 Fig. 6-4
A&B 105 60 70 Vco 60 Ic 70 NLC 105 60 70 Vce 60 Ic NL NL0 NL NL NL NL NL NLE (70 PORV) 65 80 Voe 70 Ic 70 Fig. 6-4
F (80 PORVs) 80 80Vc so k Fig. 6-4
,'S 125 70 70 Vce 60 IC 70 NL
C 125 70 70 Vce 60 kI NL NL
p NL NL NL NL NL NL
( ,0 l °,-,,-W Fig.
F (90 PORV) 90 90V08 90 IC 80 Fig. 64
NONE 6 80 60 75 Vce 751c NL NL
,PECIFIED 1 110 50 75 Vce 60 IC. 65 NL
J 110 50 75 Vce 70 IC NL NLK 125 FO 75 Vce 75 Ic NL NLL NL 50 70 Vce 70 Ic 70 NL
PA 125 NL 75 Vce 75 Ic NL NL
W NL 70 NL NL NL NL
X 125 NL 100 Vco 10010 NL NL
KEY: NL LNoUWPORV - Perwcen of Aade ViA*e
103
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Table 6-4 Silicon Bipolar Power Transistor Stress Derating Criteria
44,
4'
41
4'1
'U
-JA
104
i i i I I I I I
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6.2 G-As POW*ME TRANSISTIORS
Although both -TFTr and MOSFET styles of GaAs transistors exist, the most
common style of GaAs power trcusistor is the MESFEr. From reviews of the
available literature and supplier surveys, the primary failure mechanism for
MESFErs is the interdiffusion of the deposited xmeta-l (typically alumirum or
gold based) and the GaAs. Tyn•ically, the interdiffusion results in a
gradual degradation in performanoe due ti increased contact resistaKcl,
decreased drain current ard redched chatuxel depth.
The primary stress that accelerates this process is temperature. Table 6-5
summarizes in detail the geometry, materials, ratings and life test bias
conditions ac results obtained from various literature a-4 supplier sources
in which the effects of temperature are well documented. It is observed
that the primary failure mode has ctianged fran one that produces
catastrophic results, such as gate burn-out, to one that results in gra +-ul
energy was calculated, sucri that a lifetime prediction could be made based
on ckannel temperature. Tbese predictions are shown graphically in figure
6-2. It is noticed that, at high temperatures where the life test was
monitored, most of the re -Aences showed fairly consistent results. The
only exception was reference 154. The mean and standard deviation of the
extrapolated lifetimes from the other references enables an appruximation of
the probability of sixxess to be calculated for a given tenperature. Mae
0.5 (nean), 0.9000, 0.9900 and 0.9990 probabilities of s are shown
graphically in figure 6-3. By evaluating each curve at its intersection
with the 5 log-hour lifetime line (100,000 hours), and assuming the same
relationship between probability of success and criticality level that was
assumed for GaAs MalICs, the maximum junction temperature can be evalated
for each criticality level.. UN maxim•e m channel temperatures for GaAs power
?SFETf's are 85, 100 and 125 degrees Celsius for criticality levels I, II and
III, respectively.
105
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Table 6-5 GaAs Power MESFET Lifetest Data
A A1 A4 Ar Aj AiC, ý cL ; Z AC j(j"!: A. A-- :2 : ! A A, A1 A A,ý 5 2 C
a A3 A 0 0 C AA
cmA n( nc )c n'nmm m m i C 443" ,""c A A0 CA Z ZnAZ(
cu A'NZC% CA In~AZ~ V3 U) U) n'eJ4 3 J\3J3 S(
E Zs (/34/DAW3 Z) (3 (A C/3W A :/3 4- 0 m0 0 t0/13 ~ ( / / ~~l/M1 A) A AD A) CnA~. M CM A M - - - - - - - - 4 24 , W
OU W U4)I A) A U AK -A/C - - CA( A ( AC AK
0. S A AAm
AK AC AK AC AK AC AK -
AC A w A- -C AC -CA
A1 AA A A A A 4. .41- ~ ~ J~ A- C.AA 2A .Q A -L
AA-J-J---.-J-J4 A A A A A A A A A A A A A A A A A A A *-1 7A-j (
.C 43 ~ A W A 0 O A 0., - AO AO -Z Ao ca AA A10 AA A A AA A A A AAA0AA A A A A0 A0 10A A41 11,;C ;'I I"Ir n 1 1" nI no
03030303 ~ ~ ~ ~ ~ ~ ~ ~ a C; Aý 0300 33A 00 PAnA~ A 4 34 3 34 34
A MF - - A-
Ac 'A m~ A 44q*343J3 4334433 434 A - on "NO Anu na n U t oc ý C 01
A6 Ac C; A;8C c ;C ;C c ;C. c c ;Ao ao c Ao Q
C2 AAA
A ~~ ~ A A
If A 1 Ar A A AAIn A % Ait A LeA
A1 A Aj Aj -j co ADc mc j- 1 - j-
A. A A A) A) 0. A c' A 'Aijý j - j ý 4 Aj j4 0 A f.) . A u A)u - j j - 1-
A Ax x x A x A A ;
,:7 AA A AA A J AL A J 2
0. 0 43 - 1C 4 14C 1 JC I At A r- I- AtA* i M rn Ie fnLA L LL .. . . L L t *A
or - -/3 - -L(C4 A -UA.A A I-C .)AU.~L2 J
I A A AA A1A6
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Table 6-! GaAs Power MESFET Lifetest Data (continued)
cme
C3 a C4 It C1 a43C ýI 4- OG O C oo C, C0 - ; ; 0 I
0, 0000.000
*m 4 ,0- n D o0C3C . . -. .1 4. j -. .4-aCD. ý a 3C 4= ~ zC40 ' UN ,. K%,'
0CC~~~I (VIN'. r4__ __
O• '.0 W 0,C303.CD 000 C040000000 0 • •.*fm Cm 4q C4f
C Cm
n404 ^C OInr 24 3C ~ 4 0 C3 C: 3 4 > D0C; 40 C3 4OC ) C N 0 3 UC
4.0 1- r.- ..- r4 '0 U . n zPnIn P n r.r W%-_ f. C3 4-t. ' CO n .ý 0 . Cm
4 4 f,' 4 ,4 .' ',0. ',0'O
1- Q 4m v C4 4m f4 IN
0 r.
In •0 °0 V, • 0
'. -*.......................I - d-l- - •.•I N,.....4. . ..d...J.• d .-• , .•.,Zr....................ZZZe~t
4 -. 4f 4l V4 41 W! *4 l ýII . ..
n ! 4 i4, 0 " 0 .0 DV* 4a ID 40 40
""-J -J" -J.Jý %tU%&' ýt • -J ' -1- . t.J - - J J. .J.J J --J. J~ • • -J -•.1 OCO4
.407
*L - J- J A - II f- f- r ZZ *l -Z -1 -1Z . *. ZZ-j-j 4jt It r-j -4C; 4 r z 2 4 2
IM 4 M 1 0 v . 4
4 , a 0.00
4I Ch p Q I" In M
-' *)- P' 4 -I- CO 'l It I -'
4 2V4 :: '2.2: !2 !: r tý0.r-~..i. it..q. JJ .J.J4 Ji~.44 AI I*4 4..4.4. 44%4
~- ZZ ZZ ZZ 4 4. Z~ 4Z ZZ 4Z Zr ZZ Z0 (l~l~r107 4 4
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Table 6--5 GaAs Power MESFET Lifetest Data (continued)
l 0. m 9 C' 0 C) C3-* 4 4 4 4
(a 4 44 4 9CA m -a 4 4 en C3C4C , CýC
fn On f C4 NM-4 4J enMM4 QC)MM( O
CO O 0u2'0 * FN 0 *-0 Nf. a 0 ('J x 'O'. 0OCJ2C*.i'iO ,J
4A IT~44 IT 991 EVE.@P)4 44.4~* J4~. .~~t)4~~44) . . . . . . . ..k*
W 2 em; C4 4- =, 4LQ 4~u =4 4t L% ; u"A -n Vt f: P P : 4 C:)=JV ý - J n
! 4 4 , C, ý Q 4 W 9, L
L 2c z. Ln 4 4 L rkr 4. 0 A.n
On Fa 4 . C, 4, 4! 4 - 1p
a 4 9 4 9 c
C C)C3 C C C C 0.0 D0 00 00 C- QoaOO C5CJOO3U1 C,0
0 N 0 -4 4 ýC'
c - Vt- W10 n 0 0 W-3004000 N 6m CQOO..N'~O4. lAO at 00
40 0 4n' M9 4- 414 *
41 L % 14 n 0 gn0 4 .
C- - -L >> b
on In 44
43 4 44 4 44108.
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Figure 6-2 Lifetest Results for GaAs Power MESFUTs
I ~cm
cmJ
/ 0O
0
0) ILO
~~4)
0 I Alf
CIDI
/ I-O
0~
to 0 t
cm'
0 10 109 U
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IFigure 6--3 GaAs Power MESFET Lifetime Prediction
' •04
04 0
to
N C5
040
F-- <)
LL - .0 )0)
00
to 0 oCW Lf 0)
CC
(.O cE
2MC~N,0 C4
110-
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Supl7ementing the channel teraerature derating parameter was the stressderating paLameters ou•-lined by other derating guideline sore as 'own.n table 6-6. In keeping with the general approach outlined in Section
3.0, and because of the uncertainty of criticality assumed with guideline
sources not specifying three criticality levels, only those guideline
sources supplying derating criteria for three criticality levels were
evaluated for inclusion in the updated guidelines. For each parameter
specified by these guideline sources, a median value for the parameter was
chosen. In the case where the dcoice was between an even number of values,
the average of the two median values was calculated and then imurded up.
The remaining guideline sources were used only as a "sanity check" of the
updated stress derating criteria. From a thorough rev.iew of the
literature,- it was determined that currently accepted derating policies are
adequate in supplementing the channel temperature derating parameter inprovidiing the margins of safety and success needed for the application.
Table 6-7 summarizes the new stress derating criteria for GaAs power
transistors.
111
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Table 6-6 GaAs Power Transistor Guidelines
MAY]MUM
CHANNEL POWER BREAKOWN ONOFFCRITCALTY GUIDELINE TDISSIPATION VOLTAGE TEMPERATURELEVEL (deMPERATC) POR ORV) CYCLES
(dog C)
A&B 95 50 60 NL
c 95 50 60 NL
D 95 50 60 NLE (55 PORV) 50 60 FNg. 6-4F (55 PORV) 55 60 Fig. 6-4
A&_, 105 60 70 tA&B 105 60 70 NL
C 105 60 70 NLD 105 60 70 NL
E (70 PORV) 65 70 Fig. 6-4F (80 PORV) 80 70 Fig. 6-4
A&B 125 70 70 NL
C 125 70 70 NLD 125 70 70 NL
E (80 PORV) 80 80 Fig. 6-4F (90 PORV) 90 80 Fig. 6-4
NONE G NL NL NL NL
H NL NL NL NLSPECIFIE-D NL NL NL NL
K NL NL NL NL
L NL NL NL NLM NL NL NL NL
W 82 PORV 70 70 NL
X__ K 125iI NL J N. NL
KEY: NL - Not Listed
PORV Percent of Rated Vauue
112
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Table 6-7 GaAs Power Transistor Stress Derating criteria
U.' CO (3
4)
C4 Chn
4,1-J.
U
11
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6.3 POWER NWxFErs
MSOFETs cannot be derated in the same way as bipolar junction transistors
because the devices are constructed and operate differently. MSrS•71s have
considerably higher input impedanae than hipolar transistors, whidi makes
them suitable for microwave systems. MISFETs also have a negative
temperature coefficient at high current levels, resulting in the current
decreasing with increasing temperature. This characteristic provides for
temperature stability and prevezts the FET from thermal runaway or second
breakdown. Consequently, MISFETs have found increased acoeptanoe as power
devices.
FFrnm a thorcugh review of the literature, it was determined that currently
accepted derating policies are adequate in providing those margins of
safety and success needed for the application. The stress derating
criteria for power MOSFET transistors outlined by other derating guidelinesoures i' 5hui ln t Ir b-.epri ng. with the general approach
outlined in Section 3.0, and because of the uncertainty of criticality
assumed with guideline sources not specifying three criticality levels,
only those guideline sources supplying derating c-riteria for three
criticality levels were evaluated for inclusion in the updated guidelines.
For each parameter specified by these guideline sources, a median value for
the parmter was chosen. In the case where the choice was between an even
number of values, the average of the two median values was calculated and
then rounded up. The remaining guideline sorcs were used only as a
"sanity dceck" of the updated stress derating criteria. Table 6-9
summarizes the nev stress derating criteria for power MOSFET transistors.
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Table 6-8 Power MOSFET Transistor Guide!ines
N"Mum PO 1 SAFE SAFE BREAKDOON ON-ut F
MUNCTION PATI OPERATING OPERATING VOLTAGC TIMPERATURELEVEL.UY UII=N TEMPERATURE (FJV RAAE PO"t CYCLES
EVI. (dog C) PRV PORV), Iv (PORVV. L
A&B 95 50 NL NL 60 NL
D95 50 NI. NL 60 NL
NL NL NL NL NL NLE (55 PORV) 50 NL NL 60 Fig. e-4F (55 PC'R) 55 55 Vc 55 Ic 60 Fig.6-4
A&B 105 60 NIL NL 70 NLC 105 60 NL NL 70 NLD NL NL NL NL NL NLE (70 PORV) 66 NL NL 70 Fig. 6-4F (80 PORV) t) 80 Vce 80 Ic 70 Fig. 6-4
A&3 125 7 NIL NL 70 NLC 125 7 6 NL NL 70 NLD NL NL NL NL NL NL
Nt (80 PON so NL NL Be Fig. 6-4
_(90 _ I_ _ _ _ &0 __ vG_ __ 80 Fig. 6-4
NAJE G 60 60 75 Vce 751c NL NL
MP.CIFiED 1 -I 110 50 75 Vca &) Ic 65 NLJ 110 50 ",5 Vcc 70Ic NL NLK 125 50 (75 Vda) (75 Id) NL NiL
L NL 50 70 Vce 701c 70 NLM 125 NL PtL NL 75 NL
W NL NL. NL NL 70 NL
X 125 NL 100 Vcu 100 Ic NL NL
KEY NHI - LWdPORV P p•c og PF, V*.I
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Table 6-9 Power MOSIFET Transisqtor Stress Deratingc Criteria
-IZ
o3. itiý
4,
44
-u
L. IU
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6.4 POWER T 3ANSISTOR APPLICATION NTPES
The following application notes for power transistors were developed from a
review of applicable literature, supplier surveys and other stress derating
guidelines. Miese application notes may also be found in Apperdix A.
1. Power transistors my be sensitive to ESD.2. Design margins should be used for gain (+/- 10% for screened devices;
+/- 20% for unscreened devices), leakage cnrent (+100%), switchingtimes (+ 20%) and saturation voltage (+/- 15%).
3. Heat sinks may be required to maintain derated junction/channeltaqeratures.
4. SOA curves, adjusted for junctiorVndh l temperature, should not beexceeded under any transient conditions.
5. The number of on-off cycles (temperature cycles) shodld be limitedaccording t!he derated power as shown in figure 6-4.
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Figure 6-4 On-off Cycling Limit:., for Power/Pulse Transistors
00_______ _________0
w~2ZZZL~0
C:
+-W
(0
0,
V/)
4-0-
0
(UU
0,0
ceJ
0
0~ ) CU~ I*- (D LO Kt (9 N~ 0
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7.0 RF TRANSISTOR DERAPING GUIDELINES
RF pulse transistors and RF miultitransistor packages have typically
operated in the low microwave frequency rzge and have been largely silicon
NPN transis-tors. However, because of the advanoes in performan:ýe and
reliability of GaAs transistors, many of the siliconn RF pulse trinsistors
are being replaced by GaAs MESFETs.
Scme of the critical parameters and coxnstnrction details for RF PUke and
microwave transistors include current gain, switi time, doping level i
the base, maximum open circuit voltage (breakdown voltage) , off iixrance,
on ixpedance, emitter stripe width, base thickness package and wafer
parasitics and active area ge-imtry, includirq interdigitated, overlay and
mesh types.
Significant failure mechanisms of RF pulse transistors includes
le ." %AL"LLCL-LUII, %LJ. I..L I A .A L--t=gILt "L" -L A..L.." - LJA.I - -.La-A 0 LAfl I LriV t S.L
junction leakage and secondary breakdown. Narrow base widths can result in
collector emitter shorts due to temperature acceleratel diffusion spikes
and pipes if bulk silicon defects such as dislocations and stacking faults
are present. 'Thermal resistance problenr can occur on RF transistors and
attention to die size, die attach method, package type and application,
heat sinks and air flow are important factors relating to the derating
criteria. It is noted that the. newer device styles are 4ore powerful, more
sensitive and cover greater bandwidths, although the basic technologies are
the same. Therefore, the updated stress derating criteria for RP pulse
transistors and FF voultitxansistor packages has not changed frum the
current stress derating criteria, with the exception that perhaps greater
attention to detail is required. This attention to detail is highlighted
in the following two examples.
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In this example, a thermal runaway failurp- was cbserved in a microwave
Miltitransistor (NpN) package (see figure 7-1). .In this pacKage, two
4--transistor arrays were mounted next to each other. £lring the f.iIure
anilysis, it was detenrined that in the assembly operation, the sexradarray was not mounted properly. The array was sitting on top of the edge-
of the first array (see figure 7-2). The greatly irrzased thermal
resistance at that end of the array resulted in thermal overstress and
evet.ial !tastr1phic failure of the multitxansistor package.
-Y.-icr thzn this analysis, no additional information was accunulated on RF
nailtitransistor packages that indicated a differeme between the behavior
of pp mIultitransistor packages and RF single transistor packages.Therefol-e, it is concluded t-at the stress derating for these packages
should be no different than for PF single transistor packages. It is
reccuerled that the stress der-AtinY criteria and associated application
notes for RF transistors outlined by the current version of the Guidelines
s4hould be followed for BF irultitransistor packages.
In a seconr example, failure analysis performed on 118 RF pilse transistor
fieb,1 failures of SPS-40 transmitters identified 76 of the fuilures to be
related to MOS capacitor overvoltage, high RF voltages due to reflection,transis-.tor mismatch and thermal ireases due to reduced die attach. A
detailer thetrmal analysis idlentified war~t case junation temperatures of 87
de1.Z,••" ... l. . ihu,_ tIhh _ ruired (etrating. The RF transistors were
rated c-,t 50 volts and were not expected to see more than the transistor
emitt',--i,,ýe breakdown voltage of 6 volts. However, it was possible to
develcT) rr' vvotages across the M4S capacitors considerably higher than the
erittd-4x., k-reakdown voltage whei looking at 35 watts of palsed 450 MHz
pCwX. T • unitter-base junction breaks down without damage, but the
• it[•r• '. ?lectric breaks down as an irrevewrsible short. Good
er1i.,'w! practioes need to supplenent any deratirj policy in order to
obtAin ar. acu•erabie level of safety and success.
1.20
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FigLure 7-1 Catastrophic Damage in an RF Multitransistor Package
Figure 7-2 Assembly Problem Resulting in Thermal Runaway
L 2 1
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Although studies are being performed 16 0 - 1 6 3 to better understand the
effects of peak pulse yxxer per unit gate width, the number of pulses in a
pulse train and the duty cycle of the pulse train on the failure rate of RF
pulse transistors, the data from these studies does rot provide encNgh
insight into modifYing current stress derating guidelines for RF pulse
transistors.
The stress derating criteria for RF pulse transistors was developed
similarly to the stress derating criteria for power t-ansistors. The
chiannel teeratura stress derating developed for GaAs power MESFETs is
also considered applicable for the GaAs RF pulse transistors. The stress
der-ating criteria for RF pulse transistors outlined by other derating
guideline sources is shown in tables 7-1 and 7-2 for silicon bipolar RF
pulse transistors and GaAs pulse MESFT, respectively. In keeping with
the general approach outlined in Section 3.0, and because of the
uncertainty of criticality assumed with guideline sources rnot specifyingLLeA criticality levels, only- those - 1ide e i delr squrip yinga derating
criteria for- thre criticality levels were evaluated for inclusion in the
updated guidelines. For each parameter specified by these guideline
sources, a redian value for the parameter was chosen. In the case where
the choice was between an evem number of values, the average of the two
icdian values was calculated and then rounded up. Mhe remaining guideline
s;ources were used only as a "'sanity check" of the updated stress derating
criteria. Table 7-3 summarizes the new stress derating criteria for RF
pulse transistors.
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Table 7-1 Silicon Bipolar RF Pulse Transistor Guidelines
MAMUM PSAFE SAFE 1 ON-OFFiC• O~RA'TINO OPERAT1NG BR •
CRITICALITY JCMN DISS1PAT•ON pRAA.sT:T.A VOLTAGE TEMPERATURE(dog C)TMPJ1UFE (PORV) (PORV), Vc0 (PORV,:. I (POFN) CYCLE.
A&B 65 50 7G Vce 601 f 60 NL
C 95 50 NL NL 60 NL0 NL NL NL NL NL NL
E NL NL 70 Vce 60c C 60 FIg. 6-4F (55 PORC 55 55 Vce 5510 60 Fig. 6-4
A&S 105 60 70 VCe 60 Ic 70 NLC( 105 60 NL NL, 70 NLD NL NL NL NL NL NLE (70 PORV) NL 70 'ce GO 10 NL Fig.$-4F (80 PoRV 80 80 Vce 80 1c 70 Fig. 6-4
A& S 125 70 70 V - 60 IC 70 NLC 125 70 NL NL 70 NLD NL NL NL NL NL NLE (80 POqV) NL 70 Vca 6010 NL rI!.&-4F X ,0 SV f•,k. 6.4
G NL NL NL I NL Nt. NLSH NL NL NL NL NL' i04L
SPECIFIED j 110 50 75 Vce 70 I NL NL
K NL NL NL NL NL NLL NL 50 70 Vce 701c 70 NL
M 125 NL 75 Vce 754- NL NLW NL 70 NL NL N1- NLX NL NL NL NL NL NL
KEY; NL"NotIsidPORV - Peomn o PAb. Vakj.
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Table 7-2 GaAs RF Pulse Transistor Guidelines
t AAXIMUMCHANE POWYEn BREAKDOWN ON-OFFCRfTiCAUI"Y GUIDEUNE DISSIPATION VOLTAGE TEMPERATURE
LEVNS TEMPEPATURE (poO'PON CYCLES(dag C)
A&B 95 50 60 NLC 95 50 60 NLD 95 50 60 NLE (55 PORV) 50 60 Fig. 6-4F (55 PORV) 55 60 Fig. 6-4
A&B 105 60 70 NLc 105 Go 70 NL-D 105 60 70 NL
E (70 PORV) 65 70 Fig. 6-4F (80 PORV) 80 70 Fig. 6-4
A&B 70b I 70 NLC 125 70 70 NL
III D 125 7U 70 NLE (80 PORV) 80 80 Fig. 6-4F (90 PORV) 90 80 Fig, 6-4
G NL NL NL NLNONE H NL NL NL NLSPECIFIED i NL NL NL NL
K NL NL NL NL
L NL NL NL NL
M NL NL NL NL
W 82 PORV 70 NL
X NL NL NL NL
KEY: NL - Not st•d
PORV - Percent cif Rated Value
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Table~ 7-3 RF Pulse Transistor Stress Derating Guidelines
> 00 f-f
0m U U V% 4 002
e Lj Mi. - -. en.0t'
4m 34&U C -c
43 w
.-- - -.-
L 1254
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APPLICATION NOTES
The following application notes for RIF pulse transistors were developed
frcm a review of applicable literature, supplier surveys arld Other stress ---derating guidelines. These application notes may also be foUnd in A •Per
A.
1. PW transistors may be sensitive to ESD.2. Design margins should •_ used for gain (+/- 10% for screened devices;
+/- 20% for unscreened devices), leakage Ocrrent (100%), switchingtimes (+ 20%) and saturation voltage (+/- 15%).
3. Heat sinks may be required to maintain derated juctiorylchannelten,)eratures-
4. TMe design may require exceeding voltage and power deratixq limits,but junctionVchannel tu~erature limts should be observed at alltimes.
5. The nmber of on-off cycles (tenperature cycles) should be limitedaccording the derated power as shown in figure 6-4.
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8.0 OPIO-ELE~rIZONIC DEVICE DERATING GUIDELN
The approach to the development of the stress derating criteria for
cpto-electronic components was initiated in a fashion similar to theapproach used for silicon bipolar poxer transistors. However, it was
realized that the differences between the reliability models of
NIL-HDBK-217D Notice 1 and Mrh-HDBK-217E Notice 1 resulted in up to several
orders of magnitude difference in (improved) predicted failure rates. The
quality factor had charnged 2400% to 7000%, ard the PiT factor ofMIL-HDK-.-217E Notice 1 utilizes an activation energy of approximately one
third of the activation energy used in MIL-HDBK-217D Notice 1. The use of
the silicon bipolar power transistor approach to stress derating would have
resulted in virtually no stress derating rxquired to meet the failure rates
that were considered acceptable at the time the current version of the
Guidelines was released. As an alternative approach, the devellcpmnt of
updated "acceptable" failure rates for the three criticality levels was
considered. The failure rates that can be obtaired by applying currentlyaccepted deratirq guidelines to the reliability nmdels were deemed to be as
"acceptable" as any other values chosen. Therefore, without having to dothe failure rate calculations and the reverse stress analysis, the
currmntly accepted guidelines become the updated stress derating criteria
The stress derating criteria for cpto-electronic devices, including photo
and light emitting diodes, was developed by consensus of currnt strezs
derating guideline sources, as outlined in section 3.0. The Stressderating criteria for cpto-electronic devices cutluind by other derating
guideline sources is shown in table 8-1. In keeping with the gener-al
approach outlined in Section 3.0, and because of tne_ tuxrtainty ofcriticality assumed with guideline sources not specifying three criticality
levels, only those guideline sources suplying derating criteria for three
criticality levels were evaluated for inclusion in the updated guidelines.
Table 8-2 summarizes the new stress derating criteria for cptu-ele:tn-onic
devices.
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Table 8-1 opto-.alectronic Device Gui~de~lnes
-1 0 -4 .4 s~u~- -. 14 -j. A 4 ý -f -. j-.1 -A in -juZni '0 '
Z2f4 4, M0~ 4 1" 2,:~I4 21 Z. ZZ ;L
fn 4o 4z 411 A C >- 3 jC j - jC j- j4&A4 LA M 0Mn f- Mn 3 t;
-4 - . 4 i -j a.- j- ) 4- j
M) 0~sZ M 10Z N 7Xzz =t M *
43)
I nL -4 -1 VIi 406 t ja.-AI01 w a C)
41 ccV~
LE > 4 -Ik -j 4i 9L -1 44- L - j- i j C i-
(n 44 4
g_ 4 = -.1
,- L. I- c
C. X~t >'O :g Q~N 4
0 a4 4) 0
>4 0 4
41 444 4 128
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Table 8-2 Opto-electronic Device Stress Derating Guidelines
*4 40 4o c4 r
&A V% um t9 V4 4m a
Q5 C 40 w m m 4
L I.-4 a ~ 0 Il
44 4 4 1294 4 (.
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OP-J.X)ITMIC DEVICE A~ a ,"J'1• N NUMm
Tte fcllowirn application notes for opto-electrordc deviies were developed
from a review of sufplier surveys and othez stress derating guidelines.
These application iotes may also be found in Appendix A.
Ruoto Diodes:
1. nIie gain of APDs should be derated by 3 dB to dcc=-nt for gradualefficiexcy degradation and shiftz in the operating point.
opto-cu.ýplers:
1. External bypassing may be necessaxy to prevent damging internaloscillation due to very high gain circuitry within the opto-coupler.
2. Allow for 15% degradation in ito-coupler current transfer ratio (CIR)over the service life of the design. This degradation is especiallyprevalent at low dri.ve cxrrent. The input drive current should bewell above the turn-cn point.
Light Emitting Diodes (LEIs)
3. OQrent limiting is requirr-d (usxii a series resistor).2. Half or full wave rectified AC sine wave is rot reor-mended for LED
drive current. If rectified AC is used to drive LEDs, the peak valueof the cir-ent must- never exceed the allowable DC current maximum.
Injection Laser Diodes (1l1D.)
1. Power supplies for ILDs must be carefully designed to ccupletelye! --drete ctu _revnt prulses whaich may cause catastropic facet damage.
2. Output power should be given a 3 dB margin to acoourrt fu• yfadi-aldegradation of the device.
3. 1Reaitica1 stress, such as thernal or mecianical shock and vibration,caxue crystal lattice defects (dark lines) to grow. Stress screeningcan be used to eliminate devices with the-se defects.
4. Excess optical power of IrLs will damage facets and will destroy thedevice. Note that optical power output. is strongly teqperaturedeendent and must be monitored and controlled to assure safeoperation.
5. For SiO2 glassivated devices, the integrity of the package hermeticseal must be maintained to prevent iwLture absorption which willdegrade performance.
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9.0 PASSIVE OJ4PDNEUr DERArING GUIDELI=NS
The passive camponents of interest to this stady were hybrid deposited film
resisthrs, chip resistors (JRM) and chip capacitors, both ceramic (CDR) and
tantalum (GWR). Stress derating guidelines were developed for ttme chip
resistors aid chip capacitors only- Because no stress-failure info, mation
on hybrid deposited fiLm resistors was identified by the literature L: e rch,
supplier -LWveys, other stress derating guideline souces or accumulated
field failure data, no stress derating guidelines for hybrid deposited film
resistors onuld be developed.
The str3ss derating criteria for the chip resistor and chip capacitor was
developed fram a review of carrent stress derating guideline sources, as
outlined in section 3.0. This approach was taken after firdixq virtually
no information In the literature seardx1 6 6 - 1 6 7 concerning stress-failure
relationsmhifE of these passive camponents, and cu firmation by suppliers
that these rw~oi-ents (virtually) do not fail. Te stress derating
zritaria for these passive devices outlined by other deraticg guideline
scnrcai is sJAown in table 9-1. It is noted that none of the five guideline
scoues that typically specify three criticality levels outlined stress
derating criteria for chip capacitors. Tnerefore, the updated stress
deratirj for chip capacitors is based upon best engineering jlxiewent
biased Iy the guideline soirees prawidirg only one criticality level
c-riter ia - he stesdemratir criteria fnr ch in res-isqtn rs Ar &!vcd rrn9A in
a fastion sinilac to that for opto-electronic devices. Table 9-2
sunmarizes the now stress derating criteria for chip resistozs and chipcapacitors.
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Table 9-1 Passive Device GUidelines
U.E
C4 CU 4m
4~J2c 1c4 4
z Z* Z ;z .XO ~ 4~ Z Z
0 4 4 4
a -A - J4.4j j 4 j A4 ) j .
44)
40 i
* t44O
*2 (nI4
1.32I
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Table 9-2 Passive Device stress Derating Criteria
40 Ln Co10, Cfo
41 41
co &41 0 4
41 41
41 4
4-0
W ~ 03L L)
1331
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PASSIVE DEVICE APPLICATION NCTES
The following application notes for passive devices were developed from,;
review of supplier surveys and other stress derating guidelines. These
application notes may also be found in Appendix A.
Chip Resistors:
1. COiip resistors are sensitive to ESD.2. 11e design should tolerate a 2% shift in resistance value.3. Proper trimming 3is required to prevant latent failure in low noise
applicatiofs.4. Resistor stacking should be avoided.5. For pilse applications, the average power calculated from pulse
matnritwe, duration and repetition frequency is used to establish thepc'ter desratirq requirement.
6. Pul s matgnitude should be used to establish voltage deratingrexp~d resbant.
7. Film tentrxxtures must stay below 150 degrees Celsius.8. Voltacge stress should stay less than 2 volts/ nil.9. PadMar dc._nsity should stay lests than 200 W per square inc4,.10 Trhe effective resistance value will be reduced when used at,
frequerKies over 200 MHz because of shunt. capacitance between theresistive elenents and the connecting circuits.
Chip Cqpacitor:
1. The sin of the peak AC voltage plus any DC bias voltage must notex•c•ed the maximnm deated c4-rating voltage.
2. Prec•uticos cut-li1d in MIIr-STD-198E should be followed.3. (Ceramic) A design toierarm of +/- 12% should be allc~md.4. (Tantal•u) A design toiel oe UJ. -/ 88% shcid be alla•'•
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10. 0 SAW DERNII GUIDELINES
The stress detating criteria for SAW devices was developed frcm a review of
current stress derating guideline sources, as outlined in section 3.0.
This approach was taken after finding virtually no information in the
literature search1 69 concerning stress-failure relationships of these SAW
devices. The stress derating criteria for these SAW devices outlined by
other derating guideline sources is shcun in table 10-1. It is noted that
the four of the five guideline scurces that outline stress derating
criteria for SAW devices are split between two sets of inpxt power
derating. Therefore, the updated stress derating for SAW devices is based
upon the most recent update of these guidelines. Table 10-2 summarizes the
nsw stress derating criteria for SAW devices.
SAW DEVICE APPLICATION WYTES
The following application notes for SAW devices were develpped from a
review of sqPPlJr surveys and other stre.s demrating guidelines. rLhese
application notes may also be found in Appendix A.
1. SAW devices may be sensitive to ESD.2. Integrity of the. henretic package mst be maintained.3. The design should not subject the SAW device to the rated maximum of
shock, vibration and tenperature cycl.".
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Table 10-1 SAW Device Guidelines
C.RXAfQ INPUT POWER INPUT POWER INPUT POWER INPUT POWER OPERATINGGr'AT GUJIDELINE (< 100 MHz) (>•100 MHz) (<500 MHz) (>500 Mhz) TEMPERATURE
LEVEL (dam FML) (dBm FML) (dBm FML) (:IBm FML) (deg C)
A&13 20 10 NL NL NLC NL NL 18 13 125D NI. NL 18 13 125E 20 10 NL NL NLF NL NL NL NL NL
A&B 20 10 NL NL NL iC NL NL 18 13 125
NL NL 18 13 125
E 20 10 NL NL NLF NL NL NL NL NL
A&B 20 10 NL NL NLCNL NL I18 1ý1 125 _
HI NL NL NL 13 125ON20 10 NL NL NLF NL NL NL NL NL
G NL NL NL NL NLH NL NL NL NL NLN4ONE J NL NL NL NL NL
SPECIFIED K NL NL NL NL NLL NL NL NL NL NLM NL NL NL NL NL
W 20 10 NL NL NL -X N4L NL NL NL NL_---
KEY: NL - Not UsLd
FAL From Maximum Uimnt
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Table 10-2 SAW Device Stress Derating Criteria
EE
6
-j ÷++
4'
Z + +
1372: 1
* Qn )
4.4. 4.4.
u I
137g ~
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!1. 0 DERATING VERIFICATION
To determine the validity of the stress derating criteria, field fai!Lre
data was gathered on the ccmponent types of interest to this study.
Because of the. difficulty in verif-ying space system tailures, and the
unavailability of consistent ground based system failure data, only
avionics w-btem failure data was collected and reduced to cobserved failure
rates. Maerefore, the verification of the effectiveness of the stress
derating criteria was limited to criticality level II criteria.
The avionics systems in question included the AN/APG-66 and AN/-M-68
radars and the AIQ-131 radar jammer. The field failure data was retrieved
for the years of 1988 and 1989, in which aver 1500 sorties were flown for
each system. In reducing the data it was understood that, although the
retest OK (RMIOK failures were not included in this failure summiaxy, not
all the remaining failures were verified. This lack of verification may
reult in csrvcd failure rates that are mufch higher than actual failure
rates. Thds scenario is typically true for the resistors and capacitors
which tend to be renved along with associated suspect failed ccmponents as
a lower risk option to leaving them in place and risk another rework cycler.
Table 11-1 outlines the coq~oent types and the observed failure rates
based upon the number of failures observed and the total number of device
hours of operation each component type had experienced. It is noted that
this cbserved failure rate is based upon part removals and rn. ne•xa-ily r
verified failures. Also included in table 11-1 is the predicted failure
rate for criticality level II caxzonents. These predicted failure rates
were generated in the same fashion as the failure rates outlined in table
3-3. Table 11-2 inclWles the factor values and rationale used to geer-atethe failure rates, based on MUr-HDBK-217D Notice 1 and utilizing the stress
deratin3 criteria of the cury ent version of the Guidelines. It is cbserved
that, for the most part, the observed failure rate was ccmparable to or
less than the predicted failure rate of the coxponent. Ihe exceptionsirnluded thick film chip resistors and ceramic chip cap•acitors.
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Table 11-1 Stress Deratirig As~sessment for Level II Criticality
LO N 0 0 ON ON 0 C) r-N- VI N~ %0 CO 00 0
C-4 (NJ c-4 Sn ccý C; 0 0 0
' .ri t-' m 0 0 c
V
t o %D t r )ma
i i -I Il r(i
ONW 0 % -IAeD-40 --
'IT -( mj tI
1394
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Table 11-2 Maximum Failure Rates. For Critica~ity Level 11
'4fl~ '- 0 0 0 1 CD.4 -
41 411(%- 0 c 0 0 0
L~~~~~j- 0. ' .' 4 N 0
-' .c c2Cz .
-- -K
CL M .c cp
.C q
co f - t , Q 1
&A ~ fn M , --K >
-C -K
N, ~ ~ ~ C j CN . .
0 .41 >c * a4I E;
00
1 03
0 f 0 $4 0~' a_ _ _ _ _
I) 9- .0 0~
tj* I
0 EL a 'CL N, 4) cu -ý z; C W G d
aX U dy cc U Ne-'-
0 ~ 0 0 140
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Even if the unverified failure rates of the components are greater than
their actual failure rates, then it would be reasonable to asstume the
system design engineer has been fairly sucoessful utilizing the stress
derating criteria. However, with perhaps the exception of the RF
transistors which have a two order- of magnitude difference between observed
and expected failure rates, Iesign engineer may not be guard banding
the design more than that requ by the derating guiuelines. Therefore,
either the stress derating guidelines mast err on the conservative side or
the system design engineer must be more knowledgeable of wtiich stresses are
the most critical. In the derlopment of the updated stress derating
criteria, increased flexibility was provided in the stress derating
criteria such that the system design engineer may be more sensitive to the
way stresses affect the reliability of his design.
Based on the data of table 11-1, it is difficult to conclude that the
stress derating criteria had coupletely fulfilled its intent in keeping the
component failure rate below a specific level for the given mission
criticality. However, it is encouraging that, with the lack of
verification of the assumptions concerning the failures, the observed
failure rates are close to the expected failure rate target.
It is noted here that not all the device types listed in t,:ble 1-1 are
included in table 11-1. The failure rate analysis could not be performed
,,.• •..*'•rr.•'Y--•l •4• 4-11.�%J. % %4- .ýLd' . LA=- . L . J . C Z) I . . I .'. 4- 4=J1 1 [ .L-L
some parts (MIMICs) were not used in these systems. Second, the database
structure for part traceability depends on Westinghouse internal part
=ubers that nust be examined to determine component type (i.e., ASIC,
P"ZM, chip capp.citor, etc.). To perform this task as stated would be
costly and out of scope for this contract. Thet-efore, an alternate
approach was used to collect the failure data.
This approach first identified as many internal part numters for each
component type as possible. Then, these part numbe-rs we-e ccxqpared to the
as-designed parts list for each system. If a matcrh existed, the failure
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database was search•.-d to identify the number of failures and the total
operate tine of the component. U'fortunately, if the initial list of
caoponent internal part nmtber- was not complete, it is possible that,
alth~ough the cozxronent type was wsd in the system, it would appear as
though that couponent type was not used.
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12.0 ALTEP-N-ZCE APPROAai
It is well understood that to determirne the influence of each camwornent
failure on the criticality of a mission wunld require a catplete failure
modes and effect- analysis (F!4EA). It is also wJel1 understood that,
dependirg upcn -.. e rchitacture of a system, it is possible to have the
same style of coapnnent in two circuits of different criticality. In one
circuit, failure of the camponent ray result in total missicn failure. In
the other circuit, failure of the cnponent may resiLt in only degraded
performarce. Hawever, because the system mission is of level II
criticality, for example, the applicaticn stresses applied to both
ccanpnets are derated according to the level IT der.tiln criteria.
Actually, the mission-critical oaiponent might have been betteor dezated
according to level I criteria and the other ccx'r-onnt might bave bee•n
better deratea, acrordinj to level III criteria- By choosing Cioy level II
criteria for both ccronens, the mission is potentially in morer jeopardy
due to xcmpoent 1 and tha civnzuit design is overly constrainer due to
ccrronent 2. Unfortunately, this scenario is valid for most system
&-signs, and decidirg whicdh c-iticality level should be used tor which
ccf2onent Jn a given application is futils. An alternate approach to
stress dernting of ccmponenits that can address this dilenmma L proposd.
it is typical, early in the design rtaseA, to perform a reliability
st•yst•ms. In many' cases, t:ese allocations are flo•,,•.l doam to the 2.owest
subsystem level, the camc _ent level. At that time, trade-offs in sy-tem
architecture are made such ttat the system reliability goal may be_
achieved. Stress deratixg guidelines are utilized duri-g this design ptase
to assure mission safety eni success. Since the criticality of each
aumpon.nt on the desired Fystem mission is deperdent upox its role in
pt'formL-Kr the desired function, it is: reasonable to drate the stress on
thxat ccmpornnt according to the "mission" of the cnrponent. The level of
stress derating should therefore Le dependeit upon the acceptable failure
rate of the conponerit in its arplication.
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In order to derive stress derating criteria that is flexible erngh to be-
utilized in a domain of continuous failure rates requires the stress
derating criteria be -based on accurate reliability models. It is noted
that the updated stress derating criteria for microcirwits and MIMICs
developed as part of this stu4y was based on the updated reliability models
of MII-DESK-217F (to be published). The only differenae between the
approachi taken to update the current version of the Guidplires and this
proposed approach is the replacement of the three levels of criticality
based on system mission type with a contibuais criticality scale based on
camponent "mission".
Ths pr- lem with expanding the scope of criticality levels is identifying
and providiiV accurate values for all the vari.ables associated with
caqaieent failure. This problem is certainly apparent in the example of
microcircuits. Haoever, approximat.iLons, suLi as those used to develop the
critearia in this study, may be made that siplify arnL cornservatively bound
the deratirg criteria until mo.re acurate informatiom is available.
As described earliet 1n this report, the variables of the reliability wrodel
carl be separatead irto thrpee categories, criticality-specific,
device-specitic ard stress-specific. The criticality-specific pxamerters
included the PiE ani PiQ iactors. These factors will typically depend upon
the system mission and cannot be varied to iapprove the safety and suacess
of the ciponent missik-n. The remaining fauctors involving both
devioe-specific and stUess-specific parameters can be varied to improve the
s'afety ird sucess of the cxcponent mission.
A problc=n with evolving cxconerxt reliability models is the rxeed to
incorporate time deperdent failure itnisarams intrt these models. Sinle the
resulting failure rate is no longer constant with time, a failure rate does
notr adequately describe the nuWbr of failures tnat might be expected, that
is, the mean time between failur-es is no longer conotant. Th-efore, it
'ay be more reasonable to describe the cxurnert reliability in tenns of'a
probability of sucax-ss after a given nuqrxr of operating hours.
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Given both criticality level definition and time dependent failure rateproblems, it is still possible to define the appropriate stress derating
criteria for a ccmponent mission. However, the format in which the stress
derating criteria is to be presented may becoae tedious when presented in
table format. Figures 12-1, 12-2 and 12-3 show graphically the stress
* derating criteria SOas for component missions with probabilities of succss
of 0.9990, 0.9900 and 0.9000, respectively, for ASIC/VHSIC MNS digital
microcircuits. It is noted that because a probability of suocess is used
to generate the SOAs the xzoximm junction temperatures is no longer purely
a function of gate count, when cazqmaed to figures 4-14 throuh 4-16 in
which a constant failure rate was used to generate the SOAs.
Unfortun•tely, to obtain insight into the SOAs for c ncomoent reliability
cther than that for which these graphs were generated requires
interpolation between the grapj s. Although no suggestions are made at this
tine conceriing an acceptable table format for this data, it may bx!
advantageous for the design/reliability engineer to work from stress
derating graphs, such -s the ore presented in figures 12-1 through 12-3, or
better yet, the actual derating algorithms, in order to maintain an
understanding of the trade-offs between component complexity, applied
stress and componerit reliability.
The irportance in making the. stress derating criteria "usable" shculd nort
overwhelm the advantages in making the stress derating criteria arponent
or board "mission" critical rather than system mission critical. The
method by which system design eng 'n.• arrently employ stress derating
guidelines may have to tiange frau time consumz-iq look-ups in the tables of
strtes derating guidelike books to efficient calculations performed
concurtently on the workstation used for producing the system design.
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Figure 12--1 Ps = 0.9990 SOAs for MOS Digital ASIC/VHSIC
F- -- =1
00
- - _ - to 0\1~
0
(co0) a 0- 0
CL)
V, 0
0-
0 1L C
nunP Tl Iro I i I l I
0 c0
o ooo N- w -
146.
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Figure 12-2 Ps 0.9900 SOAs for MOS Digital ASIC/VH SIC
- T1
0
0)00C)
W0 0.4-'. 1o
co joCM- [
co- .001
4-4-
a. -
U) 75
0 U'
U")
00~I to(NJ3 o Y
1.47
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Figure 2--3 Ps 0.9000 SOAs for MOS Digital ASIC/VHSIC
' ',W ;
0
-- C)(.) Cci
o2o o
14C)
0 I I I ICL c)
> EC 0~
0
> Qoo 0
0 I
CLC
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13.0 SUMMARY
There are multiple methods by which stress deratirxg criteria can be
developed. The criteria developed during this study utilized three
methods, the use of existing reliability models, the. generation ofstress-failure relationhps based upon acumulated failure data and
onsergns of stress deratirq guidelines originating from other military and
irrlustrial facilities. Although this latter method utilizes the profound
knowledge of others, there may be no accxnming for how these criteria weredeveloped, and therefore no insight into how to modify the criteria for
charin camponent technologies and complexities. Even thuhg specificstress-failure relationships may be developed from accunulated failure
data, it is not always re&sonable to base the develoqzvnt of the stress
derating criteria on these relationships since the competing effects of the
individual stresses may not being taken into acocumt. The best method (ofthe three methods used), therefore, is the one in which current reliability
cldels are us -d S4 U-2 too %the c- fal- A . ..
This method not only allows the insight into the parameters that may beaffected by changing. component technologi•es and ccplexities, but also
ccubines the ccopeting effects of mfltiple stresses.
Unfortunately, current reliability models were not available for all the
component types described in table 1-1, arn tlerefore the other two methods
of generating stress derating criteria were used. It is noted, however,that mush effort was expezled in evaluating and attempting to update the
reliability models of the discrete ard passive caixonents. mhe literature
searches initially identified over 600 articles of which apprcocimately 240articleG were germane to this study. Of those. 240 articles, 160 articles
were. mrade available and reviewed. Forty-eight cxrponent suppliers of theseventy-two suppliers contacted also provided stxess-failure data.Unfortunately most of the data aocuxulated from these so•r•es cald not be
used to generate stress derating criteria because key elements of the
strcss-failure relatiorsliips were missing. For example, sonie sources didnot provide the time to failure, while other sources left out stress data,
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and still others neglected to provide a reference point along with the tem-
perature activation energy which is needed to describe the failure distribut-
ion.Mhe level of stress derating should be based upon the expected failure rate
provided by the reliability model. However, not all the factors that may
require derating are currently identified in the reliability model. hese
factors may include outpat current or propagation delay tim. If changes
in these factors result in changes in the observed reliability of the
carponent, then these factors also belong in the reliability molel. An
evaluation of whether the stress deratirn p identified during this
update of the Guidelines should be included in the appruiate_ reliability
model is recxrmenled. In addition, it is reocumended that an alternative
approach to stress derating, as described in section 12.0, be evaluated to
determine the advantages and disadvantages in making the stress derating
criteria ccmonent or board, 'mission" critical rather than system mission
critical.
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14.0 BIBLIOGRAPHY
1. Garry, William, et. al., 'Reliability Arnalysis/Assessment of AdvancedTecdnologies,' RADC-TRI-90-72, 1990
2. Anon, 'Simulation Is The Name Of The Game,' Electron Wireless World3. Betrano, Frank S., 'Estimating Integrated Cimziit Failure Rates From
Field Performance,' Proceedings of the Annual Reliability AndMaintainability Symposium, 1988
4. airch, Richard, Najm, Farid, Yang, Ping And Hocevar, Dale,'Pattern-indeperxient Current Estimation For Reliabilit• Analysis OfO(S Circuits,' Proceedings of the 25th ACM Design Autuaatic
Onference, 19885. Chilo, J., And Angenieux, G., 'CAD Formlars For Modeling Of Electrical
Interc ecticns In ICs,' Revue De Physique Applique6. Conrad, T.R., Mielnik, R.J. and Musolino, L.S., 'Tst I. Methodology To
Monitor And Predict Early Life Reliability Failure Mechaniss,' IE,26th Annual Proceeding-s of the IRPS, 1988
7. Cox, P., Yang, P., Mahant-Whetti, S.S. and Chatterjee, P.,'Statistical Modeling For Efficient Parametric Yield Estimation Of MOSVLSI Circuits,' IEEE Jouirnal of Solid State Circuits, 1985
8. Florescu, R.A., 'Comuents On "Extension Of The Duane PlottingTechnique, By P.S. Peck,"' IEEE Transactions on Reliability, 1986
9. Frost, David F., And Poole, Kelvin F., 'Reliant: A ReliabilityAnalysis Tool For VISI Literconnects,' I JournAl Of Solid StateCircuits, Volume 24, April, 1989
10. Hayes, J.P., 'Fault Modelin• For Digital MDS Integrated Circuits,'IEEE Transactions on Ccmputer-Aided Design of Integrated Circuits andSystems, 1984
11. Healy, J., 'Modeling IC Failure- Rates,' Procedings Of The AnnualReliability And Maintainability Symposium, 1986
12. Helms, Hward D., 'Various Architectures Of System For MeasuringEarly-life Failure Rates Of Semiconductor Ccuponents, ' rnteznationalTesting Conferux Prooeedings, 1985
13. Hightower, David, Mccusker, Deanna J., And Shuiozuka, Fazuya, 'FindingFault: An Update On Fault Sixulation,' VLSI Systems Design, October1987
14. Hbixub, D.P., NborUi, J.C., :Aa Infaat Iitality A 1- .L -te FailU-eRate Model For Electronic Equipment,' AT&T Tectmical Journzal, 1985
15. E0.o, W., 'Reliability Eancmnnt Through Cptimal Birn--in,' IEEETransactions on Reliability, 1984
16. Landis, David L., And Muha, Danial C., 'Evaluation Of System BISTUsing Canputational Performance easures,' Intemrational TestingCOaferwm. Proceedirgs, 1988
17. lee, J., Shragqwitz, E. and Sahni, S., 'A Hypercube Algorithm For The0/1 Knapsack Prblem,' International Conference On ParallelProcessing,
18. long, D.M., Jaffe, R.C. and Casey, R.H., 'Algorithm For DeterminingWorst Case Transistor Parame ters, ' IEEE Transactions on NuclearScience, 1984
19. HcGill, James, 'Predicting Hybrid Microcix•uit Reliability: A Primer,'Proceedirgs Of The 1985 Interrktional Symposium On Microelectronics,
151,
![Page 160: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/160.jpg)
20. McLeod, J., 'Sitymiation: 7-e Last Frontier,' Electronics, 198621. Morozawich, Merle, 'A Method ¶Ib Detenie Overload Safe Operating
Area,' IConference Proceedinigs Of The Intelec '85, 7th InternatioralTelexvtuiications
22. Pantic, Dragan, Denef its Of Ijrtrted Ciroitit Burn-in To obtain HighReliability Parts,' I = Transactions Or. Reliability, 1986
23. Peck, D.S, 'Egtensicn Of The Duane Plotting Technique,' IEEE.alhonxractios on Reliability, 1985
24. Rajsuman, R., Malaiya, Y.K., And Jayasuniar•a, A.P., 'On Acmracy OfSwitch-level MWxeling Of Bridging Faults In Ccuplex Gates,'Prcaedin• of the 24th ACM/IEEE Design Autnmation Conference, 1987
25. Razdari, R. and Strojwas, A.J., 'Statistical Design Raule Developer,'E Transactions On CAD Of Integrated Circuits & Systers, 1986
26. Spencer, J.L., 'Highs And Lows Of Reliability Predictions,'Prooeedirqs of the Anrual Reliability And Maintainability Symposium,1986
27. Tomaire, J.J., 'Predicting Reliability Of ISI Printed CircaitCarriers, ' Circuit World, 1986
28. Yacoub, G.Y, Pham, H., Ma, M. and Friedman, E.G., 'System For CriticalPath Analysis Based On Back Annotation And Distributed InterconnectInpedance Models,' IMicroelectron Journal,
29. Seeq Techology, Irnc-, San Jose_, CA, 'Calculation Of EEPFWK BoardMTBF,' Memory Products Reliability Notes - 1, Noverer 1987
30. Seeq Ted,.nology, Inc., San Jose, CA, 'I.C. Scale Definition,'31. inLel Corp., Santa Clara, C@, 'The_ Intel Reliability Monitor Program,'32. Intel Corp., Santa Clara, CA, 'intel Reliability Monitor Program Data
Fram 1/80 Ttrough 1/87,', Max±h 198733. Monolithic Memories, Santa Clara, CA, 'Reliability Report,', Ncvember
198334. Adams, J.H., 'Radiation Effects Ini Microelectronics For Space
Irstxvuents,' 29th Nuclear Science Synposium and 14th Syqposium OnNuclear IPower, 1983
35. Andrews, Jckvi, 'Detecting CMOS Stuck-coen Transistors,' VISI SystetoDesign, Ocboer 1987
36. Arcer, e-t al, 'A 32b CKS Microprocesscir With On-chip Instzi.ction AndAalA CAciiim_ And Me _ Management,' 1987 IEE Internaticrnal SolidState Ciaiiits Ccnference, 1987
37. Banarjee, Blioa, 'Handling The 1Aower Dissipation Of ECL Gate Arrays,'VLSI Systezc Design, Jarnary 1987
38. baze, M.P.. and Johnston, A.H., 'Testii3 Corli.&atio For RadiationIrKhiued latdhup,' I Transactions On Nuclear Science, 1987
39. PElott, B.G., 'Ganma-ray Effects On An N-c-hamnel IVS Micrtocx:ssor(Z8002) In The Zero-bias Conditi,I,' 1EETr'nsa.ctir'im. on NuclearSciernce, October 1983
40. BrowmixLg, J. S., Koga, R. and Yrolasinsk)i, W.A., 'Single Event UpsetRate Estimates For A 16-k OKS SRA4,' ILEE Tr.insaction on NuclearSciirer, 1.985
41.. Caiali, C., Fantini, F., SicKini, G., Venturi, P. and Zanoni, E.,'Bailure Modes Induced In TrL,-]S Bipolar Uigics By Negative Irnpt/s,'Alta Fregenza, 1982
152
![Page 161: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/161.jpg)
42. Canali, C., Fantini, F., Gaviraghi, S. and Senin, A., 'ReliabilityProblems In TI¶-IS Devices,' Microelectronics And Reliability, 1981
43. Chao, H.H., Ong, S., Tsai, M.Y., Shih, F.W., Hou, J.C., Lewis andK.W., 'Micro/370: A 32 Bit Sirnle-chip Microprocessor,' IEEE Jomznalof Solid State Circuits, 1986
44. Chappell, Chapell, Shuster, Seinuller, Allan, Far:± and Resti, 'FastC24S ECL Receivers With 100-wv Worst-Case Sensitivity,' IEEE JournalOf Solid State Circuits, Volume 23, 1988
45. Clatterbauhe, G.V., Weiner, J.A. and Charles, H.K. Jr., 'Gold-AluminumIrntermetallics: Ball Bond Shear Testin An Thin Film ReactionCouples,' IEEE Transactions on COomplants and Hybrids ManufacturingTect ology, 1984
46. Davies, M.S., Miles, R.E. and Postoyalko, V., 'TWo-step MethodologyFor COS VLSI Reliability Improvement: Step One,' Quality andReliability Engineering International,
47. Denton, Doanald L. And Blythe, Donald M., 'The Impact Of Burn-in On ICReliability,' Journal On Environmental Science, Jan/Feb 1986
48. Doyle, E.A., 'How Parts Fail,' IEEE Spectxm, ±98149. Dugan, M.P., 'Reloiability Characterization Of A 3-8 Micron CM0S/SOS
Process,' R- Review, 198650. Edwards, D.G., 'Testing For MOS IC Failure Modes,' IEEE Transactions
On Reliability, 198251. Enlow, E.W. and Wunsch, D.C., 'Semiconductor Failure Threshold
Estimation Problem In Electrcmagnetic Assessmeant,' E Transactionson Nuclear Science, Dec 1984
52. Fantini, F. and Marandi, C., 'Failure Modes And Mecharniswis For VLSIICs - A Review,'I EEE Proceedins, Part G, 1985
53. Ferris-Prahiu, Albert V., 'Yield Inplications And Scaling Laws ForSubmicrareter Devices,' iEEE raisactions On SancionductorManufacturing, May 1988
54. Filanovsky, Igor M. An-i Finvers, Ivaxs G., 'A Simple Nonsaturated CHOSMUltivibrator,' IIE Jcurnal Of Solid State. Circuits, Volume 23, 1988
55. Furukawa, M., Hatano, H., and Hanihara, K., 'Precisici MeasurementTechnique Of Integrated N0S Capacitor Mismatch*ing Using A SimpleOrr-cip Circuit,' IEEE Transactions on Electron Devices, 1986
56. Heath, M., Stefanakos, E., Wade, T. 1 LUller, W. and Nicolay, H., 'VLSIMultilevel Metal Defec. Qiaracterization System,' • onterencePromedings-IEEE Sactheý n, 1987
57. High Performance Systens, 'Producing Complex ASICs un TightScheduLes,' Semiconductor Design Guide, 1989
58. Hinris, D.J., Stokoe and J.C., 'Optically Induced latch-up And OtherEffects In aC'S UVEMITZMs,' Electron Letters, 1985
59. Rinode, K., Owada, N., Nishida, T. And Mukai, K., 'Stress-InducedGrain Boundary Fractures In Al-Si Intercxnnects,' Journal Of VacuumScience And Technology, B., 1987
60. lkdl, Randy And Jackson, Rick, 'Analysis Of Hiq• , ltage ESD PulseTesting On 14)S Gate Array Technology,' Electrical Ovarstrzess AndElecrostatic Discharge Syiijosium Proceedings, 1987
61. Jctnston, A.H., 'Models For Total Dose Degradation Of LinearIntgrated Circuits,' IEE Transactions on Nuclear Science, Dec 1987
153
![Page 162: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/162.jpg)
62. Kacprzak, Tcmasz, 'Arnlysis Of Oscillatory Metastable Operation Of AnRS Flip-Flop,' IEEE Jouimal Of Solid State Circuits, Volume 23, 1988
63. Kacprzak, Tamasz, Albicki, Alexander And Jackson, Todd A., 'Design OfN-well (CG Flip-Flops With Minimum Failure Rate Due ToMetastability,' IEEE International Symposium On Circuits And Systems,1986
64. Keating, Mike And Meyer, Dennis, 'A New Approach To Dynamic IDDTestings International Testirn Conference Proceedings, 1987
65. Kem, K.G. and Poole, K.F., 'Study Of Electraaigration In Double LevelMetal Syste Using Oxide And Polymer Dielectrics,' CQnferencProceedings-LEEE Sotheast-con, 1987
66. 1-jar, R.A., Lee., S.N., Parncoly, R.K. and Peel, J.L., 'Self-AlignedRadiation Aid Hard QS/ISOS, " IEEE Transactions on Nuclear Science,Dec 1976
67. KYqa, R. and Kolasinski, W.A., 'Effects Of Heavy Ions On MicrocirciitsIn Space: Recently Investigated Upset Mechanisms,, IEEE Transactionson Nuclear Science, Feb 1987
68. Kumar, M., Fissel, M.G., Pourrezaei, K., Lee, K. And Dogla, 'GrowthAnd Properties Of Tin And Ticxay Diffusion Barriers In Silicon OnSapire Integrated Circuits," Thin Solid Films, 1987
69. lee, Chen, Holland, Fong And Hu, 'Oxide Defect Density, Failure RateAnd Screen Yield,' 1986 Synposium On VLSI Technology
70. Lee, J.C., Chen, In-chin and Hu, C(enming, 'Modeling AndCharacterization Of Gate Oxide Reliability,' IEEE Transactions onElectron Devices
71. Mangir, T.E., 'Sources Of Failures And Yield IproveiPint For VLSI And•-turable Interconnects For RVISI And SI, Proceedins of the
IEEE, 198472. Mckirdy, Ray and Lea, Mike, 'WSI: A Technology For Reliability,' Yield
Modeling And Defect Tolerance In VLSI73. Meredith, John W., 'Microelectronics Reliability,' IEEE Region 5
C•nference, 198874. Miller, Jeffrey, Becht, Herbert, And Morris, Seymour, 'Akccunting For
Soft Errors In Memory Reliability Prediction,' Annual Reliability AndMaintainability Symposium, 19897" 8.•w,-- T .1 , -Tral' r'i Toadiation Effects On Various (znmercial NMSMicroprocessors,' IEEE Transactions on Nuclear Scienoe, Dec 1977
76. Olivo, Piero, Nguyen, Thao N., And Rioco, Bruno, 'High-field-inducedDegradation In Ultra-th•in Sio2 Films,' IEEE Transactions On ElectronDevices, 1988
77. Olsen, D.R., and James, K.L., 'Effects Of Ambient Atm~iospire OnAlumirrum-<4er Wirebond Reliability,' IEEE Transactions on C~mponientsand Hybrids Manufacturing Technology, 1984
78. Padcmanhan, R., 'Corrosion Failure Modes In A Tab200 Test Vehicle,'IEEE Transactions on q2onents and Hybrids Manufaacrirbi Technology,1986
79. Pantic, D.M., 'Maturity Factors In Predicting Failure Rate For LinearIntegrated CircLits,' IEEE Transactions on Reliability, 1984
80. Patterson, J.M., And David, R.F., 'An Investigation Of The Effect OfElectric Field Fquivalency (FE ) Dice Screening On Hybrid Yield,'International Symposium For Testing And Failure Analysis
154
![Page 163: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/163.jpg)
81. Pease., R.L., Turfler, R.M., Platteter, D., Emily, D. and Blice, R,'Total Dose Effects In Recessed Oxide Digital Bipolar Microcircuits,'IEEE Transactions on Nuclear Scijenýe, 1983
82. Pecht, M., Palmer, M., Schenke, W. and Porter, R., 'Investigation IntoPWB oumpcrnt-Plaoement Trade-offs,' IEEE Transactions on Reliability
83. Pesic, B., Dimitrijev, S. and Stojadinovic, N., 'Sudden FailuresAssociated With The Gate Oxide Of CMS Transistors,' MicroelectronicsReliability
84. RaCiojcic, R., 'Generic Qualification Of Semi-custcum IC ProductFamilies,' Microelectiniics Ard Reliability, 1986
85. Schroeder, J.E., Gingerich, B.L. and Bechtel, G.R., 'Total Dose andDose Rate Radiation Characterization of a Hardened EPI-C40 GateArray,' IEEE Transactions on Nuclear Science, 1984
86. Shirley, C.G. and Blish, R.C., 'Thin-film Cracking and Wire Ball ShearIn plastic Dips Due to Terperature Cycle and Thermal Shock,'Proceedings of the 25th Annual IRPS, 1987
87. Simorkaitis, D.F., 'IC Failure. Rate Estimates frcm Field Data,' IEEETransactions on CQponents and Hybrid Manufacturing Technology, 1983
88. Smith, William, Jr. and Thory, Noshir, 'Does the Burn-in of IntegratedCircuits Continue to be a Meaningful Course to Pursue,' Proceedings ofthe 38th Electronics Coaponents Conference, 1988
89. Soucair, F.S., 'High-teoperature Latchup Characteristics In VLSI CMOScircuits,' IEEE Transactions On Electron Devices, 1988
90. Stroehle, D., 'Influence Of The Chip Temperature On TheMoisb re-induced Failure Rate Of Plastic-encapsulated Devices,' IEEETransactions on Coupone-nts and Hybrids Manufacturing Technrology, 1983
91. Sweetman, Dave, And Haifley, Tim, 'Reliability Enhac•"_ients - MillionCycle EEPF4•,s,' Annual Reliability And Maintainability Synposium, 1987
92. Towner, J.M., 'Electramigration 1ýýsting Of Thin Films At The WaferLevel, ' Solid State Technology, 198A
93. Veloric, H., DT)gan, M.P., Morris, W., Denning, R. and Schnable, G.,'Reliability Of C•JS/SOS Integrated Circuits,' RCA Review, 1984
94. Winokur, P.S., Sexton, F.W. Hash, G.L. and Turpin, D.C., "Ibtal-doseFailure Mechanisms Of Integrated Circuits In Laboratory rii SpaceEnvirciients, IEEE Transactions on Nuclear Science, Dec 1987
95. Winokur, Sexton, Sdiwank, Fleetw:od, Dressendorfer and Wrobel,ITutal-duse Radiation And AnneiLing Studies: impiicaticos For iarcuness
Assurance Testing ,' IEEE Transactions Of Nuclear Science, 198696. Wittlinger, Hal, And Salerno, Carmine, 'New BiJS Process TIprves
Analog Applications: Fast, 3c,-powr Quad Op Axp Benefits FratEnhanoe~ents To High-speed CW2S,' Technological Horizons
97. Wcng, K.L., Quart, I., Yallis, J.M., and Burkhard, A.H., "CulpritsCausing Avionic Equipment Failures,' Proceedings of the AnnualReliability And Maintainability Symposium, 1987
98. Woodhall, Barnes W., Newman, B. Dale, And Sarruli, Avrid G.,'Empirical Results On Undetected Ca S Stuck-open Failures,'Proceedings of the International Testing Conference, 1987
99. Yue, H., Davison, D., Jennings, R.F., Lothongkam, P. and Rinerson, D.,'Radiation Response Of High Speed CMOS Integrated Circuits,' IEEETransactions On Nuclear Science, 1987
155
![Page 164: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/164.jpg)
100. Zietlow, T.C., Morse, T.C., Urguhart, K.C., Wil•s, K.T. and Aukerman,L., 'Correlation Of Total Dose Daange In Capacitors And Trwr-.sistors To1. 25 Micron Integrated Circuits, I IEEE Transactions on NuclearScience, Dec 1987
101. Bellem, R.D. and Jenkins, W.C., 'Radiation Effects On GaAs ChorgeCoupled Devices With High Resistivity Gate Structures,' IEEETransactions On Nuclear Science, 1986
102. Bill Roesch, 'GaAs Failure Mechanisms,' Tri-quint103. c1fristou, A. And Anand, Y., 'GaAs Mixer Diode Bunocut Mechanm At
36-94 (G{z,• IEEE, 1980104. Christou, Tseng, Peckerar, Anderson, Mc arthy, Bot, and Cawpbel,
'I!lure MiciAnsm Study Of GaAs MDDFET Devices Ard IntegratedCircuits,' IEEE, 1985
105. Fourrier, J.Y. and Pestle, J.P., 'Very High Reliability Fast bipolarIC Technology For Use In Undersea Optical Fiber Links,' Journal ofLightwave Tehnlogy, 1984
106. Fraser, Arthur, And Ogbonnah, Dominic, 'Reliability Investigation OfGaAs IC Ccaprone•trs," GaAs IC Symposium, Nov 11-14, 1985
107. Gagnon, Michael P., 'Analog GaAs ICs Show Steady Inprovement,'Electronic Products, June 15, 1988
108. Ho, Pang, Andrade, Tam, Aid Johnson, Ed, 'GaAs M4IC ReliabilityAnalysis And Its Impact On Mimwave Systems, Part I,' MSM & CT,Aug/Sept 1987
109. Larson, Lawrence E., 'High-speed Analog-to-digital Conwers& vn WithGaCks Technology_: Prospects, Trerds, And Obstacles,' IEEE Intemr-tionalSymposium On Circuits Aid Systems, 1988
110. Michael Chester, 'At The Forefront,' Electronic Products, October 15,1987
111. Peters, Michael, Roesch, William J., And Rubalcava, Anthny, 'StudyingLifetimes And Failure Rates Of C-aAs •MICs," Microe.ectronics AndRadiofrequency, July, 1988
112. Roche, J., Sasonoff, J., And Wallace, R., 'Reliable MMICs: Status AndPrpects,' Raytheon Presentation, October 21, 1988
313. Roescd, William J., '"herno-reliability Relationships Of GaAs ICs,'Gallium Arsenide IC SYnoGium, November, 1988
114. Roesch, William J., And Stunkard, Douglas, 'Proving GaAs ReliabilityWith IC Eloemnt Testing,; Triquirit Seinicouctor, 19 8.6,
115. Scaracher, Jerry, 'The Blossoming Of Digital GaAs ICs,' ElectronicProducts, June 15, 1988
116. Snodgrass, M.L. and Klinman, R., 'High Reliability High SensitivityLightwave Receiver For The SI Undersea Lightwave System,' Journal ofLightwave Technology, 1984
117. Spwdaro, Joseph J., Associate Editor, 'The Future Is Now For GaAsICs,' Electronic Products, June 15, 1988
118. Spector, M. and Dodson, G.A., 'Reliability Evaluation Of GaAs ICPre-amplifierBI C,' Techmical Digest, 1987
119. Tcrase-tta, Louis R., 'Processing Advances Push GaAs ILs To Higher VLSILevels,' EEN, June 9, 1988
120. Toq:am, P.J., Hayes, R.C., Goodridge, I.H., Tuabling, C. ani Uenn, D.,"Reterojunction Bipolar Digital ICs Using M=VD Material,' IEEEGallium Arsenide Tntegrated Circuit Symposium, 1986
156
![Page 165: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/165.jpg)
121. Wilhems n, Finn, Yee, Russell, Zee, Terry Ansi Ostrink, Nort,'Temperature 's. Reliability In Power Gaks Fi.'s And m-C GaAs FLT PowerAmplifiers,' Micrmave Journal, May 1984
122. Wirfl, J., And Hartnagel H. L., 'Field And Teperabture DepenslentLife-timn Lhniting Effects Of Metal-GaAs Interfaces Of DeviceStructures Studired By )FPS And E,' IEFI , 1986
123. Blackburn, D.L., 'Power WSFET Failure Revisited,' 19th Annual IEEEPawer Flectrorics Specialists Conferenoe, 19th, Japan, 1988
124. Black2mm, D.L. Berninq, D.W., Sanedetro, J.M. and Galiaway, K.F.,'Icnizing Radiation ELectts On Power MDSFETs During High SjpeedSwitchirmj, ' 19th Annual Conferen. e On Nu. ,ear Aid Space RadiationEffects, las Vegas, 1982
125. ainali, C. Fanirii, F., Umean, L. ani Zanoni, E., 'LeqrarlationMvdanisms Induced By Tenperature In Power MESFEBs,' ElectronicsLeLters, 1985
126. Canali, Castaldo, Fantini, Ogl.iari., Umena, And Zainil, 'GateNatllization "Sinking" Into The Active Channel In Ti/W/Au MetallizedPowar MESFETs,' IEEE Elecltron Devices tatters, 1986
127. Campenter, Grant, lea, Fred, C., Ar3 Chen, Dan Y., 'A 1800V, 300ANond1estrrtive RBSOA. Tester For Bipolar Transistors,' 19th AnnualIEEE Power Electronics Specialists Conference, April 1988
128. Chang, H.R. Baliga, E.J. Kretchrner, J.W. and Piacente, P.A.,'Insulated Gate Bipolar Triansistor (IGBT) With A Thrnth GateStrure,' Technical Digest, 1987
129. (2zng, M., Yihmhaz, H., Gauffreu, G., Hshie(n, I. and Hodgins, R.,'Advanced 50-V HLigh-side Switch Technology, ' TEEE Transactions onElectron Devices
130. DLý.s, J.M., Kcvarrec, G., Bresse, J.F.. Boulaire, J.Y. andGauieau, M., 'Investigation On Intterelectrode Yxtallic 'paths'Affecting The Operatior. Of IC MRESFErs,' Technical Digest, 1987
131. Ferla, Musuneci, 1D-atto, Spirito, And Vitale, 'SwitctingCharacter istic Of A High Voltage H4FET,' Extended Abstracts Of The.1.8th Conference On Solid State Devices And Materials, 1986
132. Fischer, T.A., 'Heavy-ion-irkuced, Gate-ruptmre In Power MCSFEIs,'=fl -rkrnctions on Nuclear Science, Dez 1987
"Reliability Of Power GaAs Field-effect Transistors,' IEEETransactions On Electron Devices, 1982
134. Fukui, Wemple, Irvin, Niehau, Hwang, Cox, Schlosser, And Dl,'Reliability Of Improved Pewer GaAs Field-effect Transistors,' IEEE,18th Procerdings Of The IRZPS, 1980
135. Gauen, Kim, Arid Schultz, Warren, 'Proper Testing Can MaximizePerformanoe In MJSFTiYs,' EIYN, May 14, 1.987
136. Ha•-t, S.A. aid Jones, B.K., 'loiw Process Yield Of Sam PNP PowerTrnwsisto.s;, ' Microelectronics Reiiabilaty
137. flu, C. and Chi, -. , kSeoomd Breakdown Of Vextical Powar IFTrsf' I'EMTransactions On Electron Devices, 1982
138. Jordar, A.S., Irvin, J.C., And Schlcsser, W.O., 'A large ScaleReliability Stiaxy Of Burnout Failure In GaAs Power FTs,' IEEE, 1980
157
![Page 166: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/166.jpg)
139. Jvanoalic, Milan M., And Lee, Fred C., 'Design Considerations ForParalleling Bipolar Transistors,' EE Transdctions For PowerElectronics, 1987
140. Kanamori, S., ani Masumoto, T., 'High-reliability Microwave SiliconPower Transistor Wit!h Stepped Electrode Struature And Tin DiffusionBarrier,' IEEE Transactions On Electron Devices, 1986
141. Kashiwagi, S., Takase, S., Usui, T. And ahono, T., 'Reliability OfHigh Frequerjc High Power GaAs-MESFETs,' IEEE, 25nd Annual ProceedigsOf The .IRPS, 1987
142. Xatsukawa, K., Kose, Y., Kanamori, M. And Sando, S., 'Reliability OfGate Metallization In Power GaeLs MESTs, ' IEEE, 22nd AnnualPrieedinrs Of The IRPS, 1984
143. Korman, C.S., Love, R.P., Ttzvp1e, V.A.K., And Walden, J.P., 'A LcwOn-resistanoe MD3FET For High Efficiency Switching Powec Supplies,'2nd InternatiokalI Conference (O Power Llectronics And Variable-seedDrives
144. nrdyanagi, Lewis, Martin, Huang, And Chen, 'Increased Degradation OfHalf-inicron PMSFErs Due To Swapped Pulse Stressing," IntemationalElectron DWices Meeting (.1E ), 1987
145. Millea, Michael F., 'Gradual Degradation Of GaAs FErs Unler NormalOperation,' 24th Annual Proceedings of the IRI-S, 1987
146. Morgan, A.N., 'Improved Power Transistoa. Perforncex By Hollt'.i EmitterConstraction - Switrlirq Pa7ne Supply Applications,' 2nd I _ternational
-fferxen-e On Ph,*nr Electronics And Variable-speed Drives147. Nakaguwa, Akio, 'Numerical Experinent For 2500V Uoible Gate
Bipolar-mcde MSFEIs (DGIGBT) And Analysis For Large Safe OperatingArea (SC1 1),' I es- 1988 RiP-cord, 19th Annual IEEE Power Electrorics"Specialists Conference, April 1988
148. Nakagawa, Akio, Yamaguchi, Yoca4dliro, And Kimtnori, Watanabe,"Improved Bipolar-mode MSFEI• (IGBT) With Self-aligning Technique AndWafer Bonding (SDB) - Why Is The Bipolar-niode M"SFET SOA,' ExtendedAbstracts Of The- 19th Cnference
149. Nakagawa, Yamaguchi, Watanabe, And Chashi, -Safe Operatirq Area For1200-V Nonlatchup Bipolar- e MOSFE-s,' IEEE Transactis On ElectronDevices1 , 1987
150. Nakatani, Y, 'Ultra-high-voltage High-speed Swit g RA- P 'er. oWith New Fine Emitter Structure,' Elex-trr Ccm=u Jpn, 1983
151. 0radin , E inc, And Praser, Arthur, 'Reliability Investigation Of 1Micron Depletion Mode IC MESFEIs,' 24th Annual Proc-eedings of theIRPS, 1986
152. Omori, Masa, And Wholey, James N., Gittons, James F., 'AcoeleratedActive Life Test Of GaAs FET And A New Failure Mode," IEEE, 1980
153. Poole, Walter, And Walshak, aIuls, 'Five-year Quest To Prove PowerTransistor Reliability,' Microwaves & Rf, July 1984
154. Russell, K.J, And EUtilmn, J.K., 'Power GaAs FEr Rf Life "st UsingTerature-aioensated Electrical Stressinx,3' IEEE, 24th AnnualProoeediixgs Of T1he IPPS, 3.986
155. SclIlarteratto, H. Ar Neubywrd, H., 'Dynamdcal Ava.anche DuringIl'rr-off Of GTO-thyristo-s And IGBTs,' Archiv Fir ElectrotechniY. 1989
158
![Page 167: ADVANCED TECHNOLOGYReliability Sciences If your address has changed or if you wish to be removed from the Rome Laboratory mailing list, or if the addressee is no longer employed by](https://reader034.vdocument.in/reader034/viewer/2022052018/6031e0e824e6ed007240f4d2/html5/thumbnails/167.jpg)
156. Schnid, Horst, 'Swi".Ii.hing Losses of The New Siret - A comparison ToOther MIdium-power Devices, ' Confxerxene Record Of The 1988Industry Applications Society Annual Meeting, 1988
157. Wada, Y., 'Electrcmigration Properties Of Titanium/AluminlLlMetallization And A Failure Mechani-so For Titaniut/Alumirnum Gate GaAsMESFET,' Journa.1 of the Electrochenical Society, 1986
158. White, P.M., Rogers, C.G. and Hewitt, B.S., 'Reliability of I.-BandGaAs rower FETs Under Highly Stressed RF Operation, JXEE, 21st AnnualProceedings of the IRPS, 1983
159. Yilmaz, Benjamin, Owyang, Cuang, And Van Dell, 'Recent Advances InInsulated Gate Bipolar Transistor (IGBT) Technology, ' ConferenceRecord Of The 1986 IEEE Industry Applications Society Annual Meeting,1986
160. Anderson, W.T., Christou, A. And Wilkins, B.R., 'GiAs FET High PowerPulse Reliability,' IEEE, 21st Annual Proceeding Of The IRPS, 1983
.61. Anderson, W.T., Buot, F.A., And Christco, A., 'High Pcnfer PulseReliability Of GaAs Power FETs," IEEE, 1986
162. James, D.S. and Dormer, L., 'A Study Of High Power PulsedCharacteristics Of Iow-noise GaAs MESFEIs, •EE Transactions OnMicro'wave Theory And Techniques, 1981
163. Yostlida, Y., Mahri, K., Yoshino, K. and Nakano, M., 'SwitchingClkiracter! -,tics And Applications Of Amorricus Ct Core Pulse TriggerydPapr Transistors (PI),' IEEE Translation Journal On Magnetics InJapan, 1985
164. Dixon, R.W., 'Current DLiections in GaAs Laser Device Development,'The Bell System T'echnical. Journal, May-June 1980
165. Spectra Diodes Labs, "101mW CW GaAlAs Laser Diode,' Data Sheet, 1989166. Munikoti, Ramhandr•a, Axd Uhar, Pulak, 'Highly Accelerated Life
Testing (HlT) For Multilayer Ceramic Capacitor Qualification,' IEEETransactions On Ccnonents, Hybrids, And M.nufacturing Technology,1988
,67. Rawal, B.S. Ladew, R. and Garcia, R., 'Facto.Ls Responsible For ThermalShock Behavior Of clip capacitors,' I Prooeedis of the 37th ElectrnicComponents Conference, 1987
168. Vale, C.R., 'Lnq 'Trem Stability of SAW 0ecoders,' IEEE UltzasonicsSymposium, 19b6
169. Colt, D.W. and Priore, M.G., 'Reliability Prediction Models ForDiscrete Semiconductor Devices,' RADC-IR-88-97, Ju.ly 1988
159
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Appendix A
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cq)
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_ 0 ML< in( L)
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00 In w .0* n 0 I I
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~1.
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4) n 4 C
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C5 W,4 < o
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co ~ 0r 1 0. f0 I
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4)4
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C , in C
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4)
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C. E
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Figure A-i On-O! f Cycl-ing Limits for Power/RF Pulse Transistors
co
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A
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Apperdix B
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C
C PROMGAM DERASICL FOJR
C Cmipute derating oarves for ASIC - MWE Digital andi Lirmearc devrices given a constant prd~ability of suc-ess or aC corstant failure rate (w~ith time). Revision 1C
IMPLICIT REAL*8 (A-11, -Z), I~rBGER*4 (I-F)CJARCTIE*80 HEADERDfl4SION VMMT(7,177) ,NEXT(7)
C Open Ir~it and Ouitput Data Files
OPEN (5, FIIE='IINPU~r. AT' I,STATUS= 'OLD')OPEN (6, FIB~'TEIW. DAV, ,STAITJSz-='NEW,')OPEN (l0,FILE=-' ',STA=S='INEW')
C ¶EVDB Constants
UOX= 8.41)0SO =0.41)0AD = .7816D5rM = 22.1)0Ea =0. 3 YJBD = 2.2221)0BM~T = 4.5D0
C biput Required Data
5 CIrXMNUEREAL (5, 200O,ENh)=50O) ITYPE, DJnM,A,PiQ, PIL, PiE,MINII,MAXTI,
* KLNH, MAXLH, NINTP, MAXrJP, INCrPVP=T (*,2000) IrfYPE,EX]M4Y,A,PiQ,PiL,Pý-F,MnINj,MAXLG,MlNIH,
* ?XTH, M=~r, MAXri, INcm
C Begin Nuznbei of Gates lrxreirnt toWpC
DO0 400 K = 0,6Cc Initialize Data ArrayC
DO0 20 I = 1,7DO0 10 J = 1, 177
NVDATA(1,J) = 0.1)C
D3-1
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10 CO~NTINUENEXT (1) =0
20 ODNTIDtJC
GATES = 10.DO**(DBLE(K)/*.2.D0) *1000.M)CC! Calculate # of Tran~sistors andi # of PinsC
TR= GAITES * 4.1)0PINS = 11.07DO * GATz- *jk 0.342D0
CC Calculate MlX, AS, Anaa iI"coe) e-ation, C1 andi C2C
'lOX = 4.931)0 / ' 0. 286W)AS = 1'349.DO TR ** O.0900CALL 7AA(A0,AS, U0,A0CrA)
CCI = 0.0100 + 0.0004271)0 * GATJE5**0.588DO
C2=2.8D)-4 * PINS**1.0800CC Begin Time Incrýrnt IocpC!
DO~ 200 J MAY'~li,MAMXISWIME DBI.E(3)TIME, = 1n.DO~**JrIF (ITYPE) 30,30,40
30 CONJ~TNJEPsmix = DUJMMYElmax = -1.1)6 * DLOG(Psmnax) /lITNEGOlDO 50
40 CrUMIUEElmax = EYM¶YPsmaX = DEXP(-1.D-6 * *~a TDIE)
50 CDNTINUECC Callculate Max Temr Frumi lambda 217F For Numl..-r of Cates andi Pins,C After (Checking For Out Of Range CordiStionC
AG= E'JjdX/(PiQ*Pi-L) - C2 * PLEIF (ARG.IE.0.D0) GWOl 150TEM'P = .DO/298.DO-DLOG(10.1)0*AIlC/C1)/ATEM4P = 1.1)0 / TIEMIP - -A73.1)0MA3CIW-1 = DINT (MI4IN I (1BLE (MAXiP) ,IW
CC Oa~t[ut Status,C
W=-TE (**)'DIV~: I, TF~i?, I Ebrawi = 1ZbaWRrITE (6,*) 'TEXP -',TM3A,' Tý1rna-x = "ma
CC 13#in Temper'ature InrcnexaKnt LoqpC
B~-2
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NEXT(J+1) = 0DO~ 100 1 = WMAX P,MAXIMP, INCrP
'IS = DBIE (I)CALL AT (TOn, S, Ea, ACCYAT)
CC Cacul~iate Failure Rate for New TeNmperature Using ?AILr-HDI3K-217FC
PiT = 0.lDO*PEXP(-A*(l.DO/(Ts+273.DO)-l.DO/298.DO))EM = PiQ * PiL * (Cl * PiT + C2 * PiE)IF (EL..GE.E~z-ax.) GOT1O 100Psac =DEXP(-1.D-6 *EL * TIME)Fcc: = 1..D0 - (Psmamx /Psac)CALL ZVAL(Fc-, Z)U =STf4E - SO* ZA(:XAEF = (10.D0**(UO -- U/AGCAA)) /AOCATM~ = DbOG (ACC2AEF) / BMl + DOV = E3 * ¶TUX * 10.1)0IF (V.GT. 18. DO) V =18. DoNEXr(J+1) = NFEcr(J+1) + 1XDATA (3+1, NEXT (J+1)) = VVDATA(1,NE-XT(J+l)) TS
100 ODM71NUEKAXI MAX (NEXT (J) N1DXT(J+1))GWOJX 200
150 0offjh1Y3EWRITE (*,*) 'ARGUMENT aJT OF RANGE'W~rMI (l0,*) 'Am2ALm2 CIT OF RANGE'
200 C0WINr~lUEC
C
'VRITE (** JJMMY,A,PiQ,PiL,PiEWR-iTE kl0,*) £UMMY,A,PiQ,PiL,PiEDO) 300 1=1, MAXI-+1
WRITE (10,1000) 'VDaTA(i,I) ,(VDMAh(J+i,I) ,J=AXUI,MAXLH)300 om~400 CX~?iNhUE
500 STOPCC JFornat Statemm~t.,-C
1,000 FOIRXT (lX, 71F10.22000 FORMAT (12,G9.4,4G8.2,715)
b3-3
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IU31 WE AA(AO,AS, TUO,AOC)C
CC SUMi1INE A:CC JPURPOE:CC Calculate the acceleration factor due to dielectric areaC relative to a reference area.CC USAGE:CC CALL AA (AO,ASUO,ACC)CC DESCRIMfION OF PARAMETERS:CC AO - referer~e area (square microns)C AS - operating area (square microns)C UO - log of median t•hi of reference distribution (hours)C ACC - acceleration factorCC SUPROJTITNBE AND FUNCTION S7JBPROGRAMS RIDJTPED:CC Z•AL - calculates number of sigmas frctu the meanC
CT1PLCTI' REAI,*8 (A--H,O-Z), ITITER*4 (I-N)F = AO / (AO + AS)CALL ZVAL(F, Z)AOC = 1. W + (Z / UW)
END
B-4
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SUMRUrXTINE AT (TO, TS, Ea, ,AGC)C
CC SUBRUTINE ATCC PRPROSE:Co Calculate the acceleration factor due to tarperature stressC relative to a reference tenpezatu'e-CC USAGE:Co CAlL AT ('ID,Th,,Ea,AOC)CC DESOCRP1TtON OF PARIAMETRaS:CC 110 - reference temperatureC TIS - opeiLating teupenatureo Ea -activation energy, (eV/dag K)C A(X - acre-leration factorCc SUBRUbXrIE A14D FUNCTON SUBFCCX-RAIC RDQUIRED:CC NONEC
CIMPLICIT I-EAL*8 (A-H-,0O-Z), 1NIEGERfl*4 (1-N)B = 8.617D--5ACC = DIX( (Ea/L-')*(1.DO/(¶fl2*273.DQ) - 1.,DO/(TS+273..DO)))PEIYJEN'nm
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SUBRYJTINE ZVAL (F, Z)C
CC SUNCUTINE ZVAL~CC PROECC Calculates the number of sigmas away frcmi the mean of aC normal distribuation~ for a given prdoability of failureC (cunilative percent failure in decimal) . This subrcaitibeeC uses the Newton-Paphson methodi of finding~ roots.CC USAGE:CC CALL ZVAL(F, Z)CC DESCIPTION OF PAFPA1EThRS:CC F - probability of failure (canmrlative percent failure inC decimal)C Z - number of sigmas from the me-an of the norffal distributionCC StJBXflJNS AND FUNCrION SUBPiRJGRAIIS REYQ=RE:CC M~A. - cumulative- normlal distribuition approxinationC
CThPUCI PEL*8 (A-H,O-Z), INTDMER*4 (I-N)
CIF (F.I.E.O.SD0) ZNE'W = -O.5D0IF (F.GT.O.5DO) ZNEW = 0.5W~Z = ZNaW
CDO 5 N=-!, 00
IF (IF AG.EXQ.-l) I4FN - O.IX)IT (M~AG.MX.1) flTEW =l.DORII = FNEFPiIP4I = l.DO/(c6QlrT(2.DO*3.141592653589793)*D)EXP(.500*z**2))ZNLV = ZZ=Z - PM¶i / HIR-ItrIF (DAWES(Z-ZNEW)/flBS(Z) .11. 0. OOQOOlODO) RFIURN
5 CflMTNUERL'I1M
END-
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tE:4X-INE Q4NDA (Z, F, IFIAG)C
CC SU1BJI'INE CNE)ACC PURRPSE:CC Calculates the value of the cumulative normal distribution atC a given number of sigmas away from the mean. This subroutineC uses a series expansion of the normal distribution to performC the integration.CC USAGE:CC CALL C4DA (Z,F,IFIA)CC DEFI=ON OF PARAMEr:CC Z - nnber of signias frcm the mean = (x - u) /sC F - area under the normal distribution at ZC IFLAG - error flag= 0 OKC -- 1 Z is less than -5. 5C -1 Z is greater than 5.5CC SUBRO=IES AND SUBPROGRAM RBQUIRED:CC NONEC
CIMPLICIT REAL*8 (A-H,O-Z), INTEGER*4 (I-N)N= 0F = O.DO
C1'TrT Ar
IF (Z.Gr.5.5D0) IFLAG = 1IF (Z.LT.-5.5D0) IFtAC = -1IF (I-TAG.NE.0) RPJARN
C1 FAUr = 1.DO
DO 3 N=0,135RN = NIF (N.EQ.0) GO 110 2FACT = FAC' * RN
2 SUMN = (-l.DO)**N * Z**(2*N41)SLUAD = (2.D0*RN41.DO) * 2.DO**N A FACTsW = SUN / SUNDF = F + SUM
3 cou ill".1F = F / 1X3QR1(2.Do * 3.141592653589793) + 0.5D0REIUININD
"-3-7
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MISSION
OF
ROME LABORATORY
Rome Laboratory plans and executes an interdisciplinary program in re-
search, development, test, and technology transition in support of Air
Force Command, Control, Communications and Intelligence (C31) activities
for all Air Force platforms. It also executes selected acquisition programs
n several, ureu., of expertise. Technical and engineering support within
areas of competence is provided to ESD Program Offices (POs) and other
ESD elements to perform effective acquisition of C031 systems. In addition,
Rome Laboratory's technology supports other AFSC Product Divisions, the
Air Force user community, and other DOD and non-DOD agencies. Rome
Laboratory maintains technical competence and research prcgrams in areas
including, but not limited to, corn munications, command and control, battlemanagement, intelligence information proeessinjq, computational sciences
~ and software producibility, wide area surveillance/sensors, signal proces-
sing, solid state sciences, photonics, electromagnetic technology, super-
conductivity, and ea .tronic reliAbility/maintainability and testability.