Probabilistic Soft Error Rate Estimation from Statistical SEU Parameters

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Probabilistic Soft Error Rate Estimation from Statistical SEU Parameters

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Probabilistic Soft Error Rate Estimation from Statistical SEU Parameters Fan Wang* Vishwani D. Agrawal Department of Electrical and Computer Engineering –

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Title: Probabilistic Soft Error Rate Estimation from Statistical SEU Parameters


1
Probabilistic Soft Error Rate Estimation from
Statistical SEU Parameters Fan Wang Vishwani
D. Agrawal
Department of Electrical and Computer
Engineering Auburn University, AL 36849
USA Presently with Juniper Networks, Sunnyvale,
CA
17 th IEEE North Atlantic Test Workshop
2
Outline
  • Background
  • Problem Statement
  • Analysis
  • Results and Discussion
  • Conclusion

3
Motivation for This Work
  • With the continuous downscaling of CMOS
    technologies, the device reliability has become a
    major bottleneck.
  • Sensitivity of electronic systems can potentially
    become a major cause of soft (non-permanent)
    failures.
  • There is no comprehensive work that considers all
    factors that influence soft error rate.

4
Strike Changes State of a Single Bit
a-particle or high-energy neutron
Logic or Memory Device
0
1
Definition from NASA Thesaurus Single Event
Upset (SEU) Radiation-induced errors in
microelectronic circuits caused when charged
particles also, high energy particles (usually
from the radiation belts or from cosmic rays)
lose energy by ionizing the medium through which
they pass, leaving behind a wake of electron-hole
pairs.
5
Impact of Neutron Strike on a Silicon Transistor
neutron strike
Strikes release electron hole pairs that can be
absorbed by source drain to alter the state of
the device


-


-
-
-
Transistor Device
  • Neutron is a major cause of electronic failures
    at ground level.
  • Another source of upsets alpha particles from
    impurities in packaging materials.

6
Cosmic Rays
Source Ziegler et al.
  • Neutron flux is dependent on altitude,
    longitude, solar activity etc.

7
Problem Statement
  • Given background environment data
  • Neutron flux
  • Background energy (LET) distribution
  • These two factors are location-dependent.
  • Given circuit characteristics
  • Technology
  • Circuit netlist
  • Circuit node sensitive region data
  • These three factors are circuit-dependent.
  • Estimate soft error rate in standard FIT units.
  • Linear Energy Transfer (LET) is a measure of the
    energy transferred to the device per unit length
    as an ionizing particle travels through material.
    Unit MeV-cm2/mg.
  • Failures In Time (FIT) Number of failures per
    109 device hours

8
Measured Environmental Data
  • Typical ground-level neutron flux 56.5cm-2s-1.
  • J. F. Ziegler, Terrestrial cosmic rays, IBM
    Journal of Research and Development, vol. 40, no.
    1, pp. 19.39, 1996.
  • Particle energy distribution at ground-level
  • For both 0.5µm and 0.35µm CMOS technology
    at ground level, the largest population has an
    LET of 20 MeV-cm2/mg or less. Particles with
    energy greater than 30 MeV-cm2/mg are exceedingly
    rare.
  • K. J. Hass and J. W. Ambles, Single Event
    Transients in Deep Submicron CMOS, Proc. 42nd
    Midwest Symposium on Circuits and Systems, vol.
    1, 1999.

Probability density
0 15 30
Linear energy transfer (LET), MeV-cm2/mg
9
Proposed Soft Error Model
10
Pulse Widths Probability Density Propagation
fX(x)
Delay tp
fY(y)
  • We use a 3-interval piecewise linear
    propagation model
  • Non-propagation, if Din tp.
  • Propagation with attenuation, iftp lt Din lt 2tp.
  • Propagation with no attenuation, if Din ? 2tp.
  • Where
  • Din input pulse width
  • Dout output pulse width
  • tp gate input output delay

11
Validating Propagation Model Using HSPICE
Simulation
  • Simulation of a CMOS inverter in TSMC035
    technology with load capacitance 10fF

12
  • Pulse Width Density Propagation Through a CMOS
    Inverter

13
Soft Error Occurrence Rate Calculation for
Generic Gate
14
Comparing Methods of Analysis
Factors Considered LET Spec. ReconvFanout Sens. region Occurance rate Vectors ? Altitude Ckt Tech. SET degrad
Our work Yes No Yes Yes No Yes Yes Yes
Rao et at. 1 Yes No No No Yes Yes Yes Yes
Rajaraman et al. 2 No No No No Yes No No Yes
Asadi-Tahoori 3 No No No Yes No No No No
Zhang-Shanbhag4 Yes No Yes Yes Yes Yes Yes No
Rejimon-Bhanja 5 No No No Yes Yes No No No
15
Experimental Result Comparison
Ckt PI PO Gates Our approach Our approach Rao et al. 1 Rao et al. 1 Rajaraman et al2 Rajaraman et al2
Ckt PI PO Gates CPU s FIT CPU s FIT CPU min Error Prob.
C432 36 7 160 0.04 1.18x103 lt0.01 1.75x10-5 108 0.0725
C499 41 32 202 0.14 1.41x103 0.01 6.26x10-5 216 0.0041
C880 60 26 383 0.08 3.86x103 0.01 6.07x10-5 102 0.0188
C1908 33 25 880 1.14 1.63x104 0.01 7.50x10-5 1073 0.0011
Computing Platform Computing Platform Computing Platform Computing Platform Sun Fire 280R Sun Fire 280R Pentium 2.4 GHz Pentium 2.4 GHz Sun Fire v210 Sun Fire v210
Circuit Technology Circuit Technology Circuit Technology Circuit Technology TSMC035 TSMC035 Std. 0.13 µm Std. 0.13 µm 70nm BPTM 70nm BPTM
Altitude Altitude Altitude Altitude Ground Ground Ground Ground N/A N/A
BPTM Berkley Predictive Technology Model
16
More Result Comparison
Measured Data Measured Data Logic Circuit SER Estimation Ground Level Logic Circuit SER Estimation Ground Level
Devices SER (FIT/Mbit) Our Work Rao et al. 1
0.13µ SRAMs6 10,000 to 100,000 1,000 to 10,000 1x10-5 to 8x10-5
SRAMs, 0.25µ and below 7 10,000 to 100,000 1,000 to 10,000 1x10-5 to 8x10-5
1 Gbit memory in 0.25µ 8 4,200 1,000 to 10,000 1x10-5 to 8x10-5
The altitude is not mentioned for these data.
17
Discussion
  • We take the energy of neutron to be the key
    factor to induce SEU. In real cases, there can
    also be secondary particles generated through
    interaction with neutrons.
  • Estimating sensitive regions in silicon is a hard
    task. Also, the polarity of SET should be taken
    into account.
  • Because on the earth surface, typical error rates
    are very small, their measurement is time
    consuming and can produce large discrepancy. This
    motivates the use of analytical methods.
  • For example, a circuit may experience 1
    SEU in 6 months (4320 hours), equals 231,480 FIT.
    It is also likely that the circuit has 0 SEU in
    these 6 months, so the measured SER is 0 FIT.

18
Discussion Continued
  • Fan-out stems should be considered. Two
    situations can arise
  • When an SET goes through a large fan-out, the
    large load capacitance can eliminate the SET, or
  • If it is not canceled by the fan-out node, it
    will go through multiple fan-out paths to
    increase the SER.
  • It is highly recommended to have more field tests
    for logic circuits.
  • None of these SER approaches consider the process
    variation effects on SER.
  • Without consideration of electrical masking, SER
    will be overestimated by 138 for a small 5-stage
    circuit Wang et al., VLSID07
  • Intra-die threshold voltage variation can result
    in a peak to peak SER variation of 41 in a small
    circuit Ramakrishnan et al., ISQED07

19
Conclusion
  • SER in logic and memory chips will continue to
    increase as devices become more sensitive to soft
    errors at sea level.
  • By modeling the soft errors by two parameters,
    the occurrence rate and single event transient
    pulse width density, we are able to effectively
    account for the electrical masking of circuit.
  • Our approach considers more factors and thus
    gives more realistic soft error rate estimation.

20
References
  • 1 R. R. Rao, K. Chopra, D. Blaauw, and D.
    Sylvester, An Efficient Static Algorithm for
    Computing the Soft Error Rates of Combinational
    Circuits," Proc. Design Automation and Test in
    Europe Conf., 2006, pp. 164-169.
  • 2 R. Rajaraman, J. S. Kim, N. Vijaykrishnan,
    Y. Xie, and M. J. Irwin, SEAT-LA A Soft Error
    Analysis Tool for Combinational Logic,", Proc.
    19th International Conference on VLSI Design,
    2006, pp. 499-502.
  • 3 G. Asadi and M. B. Tahoori, An Accurate
    SER Estimation Method Based on Propagation
    Probability, Proc. Design Automation and Test in
    Europe Conf.,2005, pp. 306-307.
  • 4 M. Zhang and N. R. Shanbhag, A Soft Error
    Rate Analysis (SERA) Methodology," Proc. IEEE/ACM
    International Conference on Computer Aided
    Design, ICCAD-2004, 2004, pp. 111-118.
  • 5 T. Rejimon and S. Bhanja, An Accurate
    Probabilistic Model for Error Detection," Proc.
    18th International Conference on VLSI Design,
    2005, pp. 717-722.
  • 6 J. Graham, Soft Errors a Problem as SRAM
    Geometries Shrink, http//www.ebnews.com/story/OEG
    20020128S0079, ebn, 28 Jan 2002.
  • 7 W. Leung F.-C. Hsu Jones, M. E., "The
    Ideal SoC Memory 1T-SRAMTM," Proc. 13th Annual
    IEEE International on ASIC/SOC Conference, 2000,
    pp. 32-36.
  • 8 Report, Soft Errors in Electronic
    Memory-A White Paper," Technical report, Tezzaron
    Semiconductor, 2004.
  • 9 F. Wang and V. D. Agrawal, Sngle Event
    Upset An Embedded Tutorial, Proc. 21st
    International Conf. VLSI Design, 2008, pp.
    429-434.
  • 10 F. Wang and V. D. Agrawal, Soft Error Rate
    Determination for Nanometer CMOS VLSI Logic,
    Proc. 40th Southeastern Symp. System Theory,
    2008, 324-328.
  • 9 F. Wang, Soft Error Rate Determination for
    Nanometer CMOS VLSI Circuits, Masters Thesis,
    Auburn University, May 2008.

21
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