SBOK052 May   2024 OPA4H014-SEP

 

  1.   1
  2.   OPA4H014-SEP Single-Event Latch-Up (SEL) Radiation Report
  3.   Trademarks
  4. 1Overview
  5. 2SEE Mechanisms
  6. 3Irradiation Facilities and Telemetry
  7. 4Test Device and Test Board Information
    1. 4.1 Qualification Devices and Test Board
    2. 4.2 Characterization Devices and Test Boards
  8. 5Results
    1. 5.1 SEL Qualification Results
    2. 5.2 SET Characterization Results: TAMU K500 Cyclotron
    3. 5.3 SEE Characterization Results: MSU FRIB Linac
    4. 5.4 Analysis
    5. 5.5 Weibull Fit
  9. 6Summary
  10.   A TAMU Results Appendix
  11.   B MSU Results Appendix
  12.   C Confidence Interval Calculations
  13.   D References

C Confidence Interval Calculations

For conventional products where hundreds of failures are seen during a single exposure, one can determine the average failure rate of parts being tested in a heavy-ion beam as a function of fluence with high degree of certainty and reasonably tight standard deviation, and as a result, have confidence that the calculated cross-section is accurate.

With radiation-hardened parts however, it is difficult to determine the cross-section because often few or no failures are observed during an entire exposure. Determining the cross-section using an average failure rate with standard deviation is no longer a viable option, and the common practice of assuming a single error occurred at the conclusion of a null-result can result in a greatly underestimated cross-section.

In cases where observed failures are rare or non-existent, the use of confidence intervals and the chi-squared distribution is indicated. The chi-squared distribution is particularly designed for the determination of a reliability level when the failures occur at a constant rate. In the case of SEE testing where the ion events are random in time and position within the irradiation area, a failure rate is expected that is independent of time (presuming that parametric shifts induced by the total ionizing dose do not affect the failure rate), and as a result, the use of chi-squared statistical techniques is valid (because events are rare, an exponential or Poisson distribution is used).

In a typical SEE experiment, the device-under-test (DUT) is exposed to a known, fixed fluence (ions / cm2) while the DUT is monitored for failures. This is analogous to fixed-time reliability testing and, more specifically, time-terminated testing where the reliability test is terminated after a fixed amount of time whether or not a failure has occurred (in the case of SEE tests fluence is substituted for time and hence it is a fixed fluence test (6)). Calculating a confidence interval specifically provides a range of values which is likely to contain the parameter of interest (the actual number of failures per fluence). Confidence intervals are constructed at a specific confidence level. For example, a 95% confidence level implies that if a given number of units were sampled numerous times and a confidence interval estimated for each test, the resulting set of confidence intervals can bracket the true population parameter in about 95% of the cases.

To estimate the cross-section from a null-result (no fails observed for a given fluence) with a confidence interval, start with the standard reliability determination of lower-bound (minimum) mean-time-to-failure for fixed-time testing (an exponential distribution is assumed) in Equation 3:

Equation 3. M T T F = 2 n T χ 2 ( d + 1 ) ; 100 ( 1 - α 2 ) 2

Where:

  • MTTF is the minimum (lower-bound) mean-time-to-failure,
  • n is the number of units tested (presuming each unit is tested under identical conditions),
  • T is the test time,
  • and χ2 is the chi-square distribution evaluated at 100(1 – α / 2) confidence level
  • d is the degrees-of-freedom (the number of failures observed).
With slight modification for our purposes we invert the inequality and substitute F (fluence) in the place of T as shown in Equation 4:

Equation 4. M F T F = 2 n F χ 2 ( d + 1 ) ; 100 ( 1 - α 2 ) 2

Where:

  • MFTF is mean-fluence-to-failure
  • F is the test fluence
  • Χ2 is the chi-square distribution evaluated at 100(1 – α / 2) confidence
  • d is the degrees-of-freedom (the number of failures observed).
The inverse relation between MTTF and failure rate is mirrored with the MFTF. Thus the upper-bound cross-section is obtained by inverting the MFTF as shown in Equation 5:

Equation 5. σ = χ 2 ( d + 1 ) ; 100 ( 1 - α 2 ) 2 2 n F

Assume that all tests are terminated at a total fluence of 106 ions/cm2. Assume there are a number of devices with different performances that are tested under identical conditions. Assume a 95% confidence level (σ = 0.05). Note that as d increases from 0 events to 100 events, the actual confidence interval becomes smaller, which indicates that the range of values of the true value of the population parameter (in this case, the cross-section) is approaching the mean value + 1 standard deviation. As more events are observed, the statistics are improved such that uncertainty in the actual device performance is reduced.

Table C-1 Experimental Example Calculation of MFTF and σ Using a 95% Confidence Interval(1)
Degrees-of-Freedom (d) 2(d + 1) χ2 at 95% Calculated Cross-Section (cm2)
Upper-Bound at 95% Confidence Mean Average + Standard Deviation
0 2 7.38 3.69E–06 0.00E+00 0.00E+00
1 4 11.14 5.57E–06 1.00E–06 2.00E–06
2 6 14.45 7.22E–06 2.00E–06 3.41E–06
3 8 17.53 8.77E–06 3.00E–06 4.73E–06
4 10 20.48 1.02E–05 4.00E–06 6.00E–06
5 12 23.34 1.17E–05 5.00E–06 7.24E–06
10 22 36.78 1.84E–05 1.00E–05 1.32E–05
50 102 131.84 6.59E–05 5.00E–05 5.71E–05
100 202 243.25 1.22E–04 1.00E–04 1.10E–04
(1) Using a 95% confidence interval for several different observed results (d = 0, 1, 2,…100 observed events during fixed-fluence tests) assuming 106 ions / cm2 for each test. Note that as the number of observed events increases the confidence interval approaches the mean.