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May 14-16, 2008 NATW'2008 1 Probabilistic Soft Error Rate Estimation from Statistical SEU Parameters Fan Wang* Vishwani D. Agrawal Department of Electrical.

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Presentation on theme: "May 14-16, 2008 NATW'2008 1 Probabilistic Soft Error Rate Estimation from Statistical SEU Parameters Fan Wang* Vishwani D. Agrawal Department of Electrical."— Presentation transcript:

1 May 14-16, 2008 NATW'2008 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 May 14-16, 2008 NATW'2008 2 Outline  Background  Problem Statement  Analysis  Results and Discussion  Conclusion

3 May 14-16, 2008 NATW'2008 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 May 14-16, 2008 NATW'2008 4 Strike Changes State of a Single Bit Logic or Memory Device 01 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. ” α -particle or high-energy neutron

5 May 14-16, 2008 NATW'2008 5 Impact of Neutron Strike on a Silicon Transistor  Neutron is a major cause of electronic failures at ground level.  Another source of upsets: alpha particles from impurities in packaging materials. Strikes release electron & hole pairs that can be absorbed by source & drain to alter the state of the device + - + + + - - - Transistor Device source drain neutron strike

6 May 14-16, 2008 NATW'2008 6 Cosmic Rays Earth’s Surface p n p p n n p p n n n  Neutron flux is dependent on altitude, longitude, solar activity etc. Source: Ziegler et al.

7 May 14-16, 2008 NATW'2008 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-cm 2 /mg. **Failures In Time (FIT): Number of failures per 10 9 device hours

8 May 14-16, 2008 NATW'2008 8 Measured Environmental Data   Typical ground-level neutron flux: 56.5cm -2 s -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-cm 2 /mg or less. Particles with energy greater than 30 MeV-cm 2 /mg are exceedingly rare.”   K. J. Hass and J. W. Ambles, “Single Event Transients in Deep Submicron CMOS,” Proc. 42 nd Midwest Symposium on Circuits and Systems, vol. 1, 1999. Linear energy transfer (LET), MeV-cm 2 /mg Probability density 0 15 30

9 May 14-16, 2008 NATW'2008 9 Proposed Soft Error Model Occurrence rate

10 May 14-16, 2008 NATW'2008 10 Pulse Widths Probability Density Propagation 1 X Y We use a “3-interval piecewise linear” propagation model 1) Non-propagation, if D in ≤τ p. 2) Propagation with attenuation, ifτ p < D in < 2τ p. 3) Propagation with no attenuation, if D in  2τ p. Where  D in : input pulse width  D out : output pulse width  τ p : gate input output delay τpτp 2τp2τp 0D in D out f X (x) f Y (y) Delay τ p

11 May 14-16, 2008 NATW'2008 11 Validating Propagation Model Using HSPICE Simulation  Simulation of a CMOS inverter in TSMC035 technology with load capacitance 10fF

12 May 14-16, 2008 NATW'2008 12 Pulse Width Density Propagation Through a CMOS Inverter

13 May 14-16, 2008 NATW'2008 13 Soft Error Occurrence Rate Calculation for Generic Gate

14 May 14-16, 2008 NATW'2008 14 Comparing Methods of Analysis Factors Considered LET Spec. Reconv Fanout Sens. region Occur ance rate Vectors ? Altitude Ckt Tech. SET degrad Our workYesNoYesYesNoYesYesYes Rao et at. [1]YesNoNoNoYesYesYesYes Rajaraman et al. [2]NoNoNoNoYesNoNoYes Asadi-Tahoori [3]NoNoNoYesNoNoNoNo Zhang- Shanbhag[4]YesNoYesYesYesYesYesNo Rejimon- Bhanja [5]NoNoNoYesYesNoNoNo

15 May 14-16, 2008 NATW'2008 15 Experimental Result Comparison Ckt # PI # PO # Gat es Our approachRao et al. [1] Rajaraman et al[2] CPU s FIT CPU s FIT CPU min Error Prob. C4323671600.041.18x10 3 <0.011.75x10 -5 1080.0725 C49941322020.141.41x10 3 0.016.26x10 -5 2160.0041 C88060263830.083.86x10 3 0.016.07x10 -5 1020.0188 C190833258801.141.63x10 4 0.017.50x10 -5 10730.0011 Computing PlatformSun Fire 280RPentium 2.4 GHz Sun Fire v210 Circuit TechnologyTSMC035Std. 0.13 µm70nm BPTM* AltitudeGround N/A *BPTM: Berkley Predictive Technology Model

16 May 14-16, 2008 NATW'2008 16 More Result Comparison Measured Data Logic Circuit SER Estimation Ground Level Devices SER* (FIT/Mbit) Our WorkRao et al. [1] 0.13µ SRAMs[6] 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 Gbit memory in 0.25µ [8] 4,200 * The altitude is not mentioned for these data.

17 May 14-16, 2008 NATW'2008 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. 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 May 14-16, 2008 NATW'2008 18  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., VLSID’07]  Intra-die threshold voltage variation can result in a peak to peak SER variation of 41% in a small circuit [Ramakrishnan et al., ISQED’07] Discussion Continued

19 May 14-16, 2008 NATW'2008 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 May 14-16, 2008 NATW'2008 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. 19 th 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/OEG20020128S0079, ebn, 28 Jan 2002. [7] W. Leung; F.-C. Hsu; Jones, M. E., "The Ideal SoC Memory: 1T-SRAM TM," 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,” Master’s Thesis, Auburn University, May 2008.

21 May 14-16, 2008 NATW'2008 21 Thank You...


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