SLVK244 January 2026 TRF0213-SEP
The TRF0213-SEP was characterized for SETs from 1.42 to 56.1MeV-cm2/mg (refer to Table 5-1) at +5V, +5.5V supply voltages. The device was tested at room temperature for all SETs runs. Since the TRF0213-SEP is a flip chip device, the devices were thinned to 50µm for proper heavy-ion penetration into the active circuits. Flux of 104 (most used) ions/cm2-s and fluence of 2 x 106 ions/cm2 per run were used during the heavy ion characterization. The devices were tested under dynamic (AC) inputs (as described in Section 6). The SETs discussed in this report were defined as output voltages excursion that exceed a window trigger set on the MSO58B. Outputs of the TRF0213-SEP were converted to SE using HL9404 balun and monitored. Test conditions used during the testing are presented in Table 8-1. Weibull-Fit and cross section for Unit #4 are presented in Figure 8-1. To calculate the cross section values at different supply voltages the total number of upsets (or transients) and the fluences where combined (add together) by LETEFF to calculate the upper bound cross section (as discussed in Single-Event Effects Confidence Interval Calculations) at 95% confidence interval. The σPERCASE (each row is a case) cross section presented in Table 8-1, was calculated using the MTBF method at 95% confidence. For the SET test, upsets were observed when setting the window trigger to ±20mV and monitoring the output of the balun. Worst case AC upset is shown in Figure 8-2. Though not observed during the testing, note that an SET event can result in output going up to saturation voltage. It was observed that all events recovered in less than 200ns throughout the testing period.
The upper-bound SET cross-sections (σALL) was calculated using the events and fluences. Cross-section points for each case are plotted in Figure 8-1 while the Weibull curve fit is generated only using VDD = 5V cases. Using the MTBF method at 95% confidence interval (see Single-Event Effects Confidence Interval Calculations for a discussion of the MTBF cross section calculation method), the combined upper bound cross section is:
σSET-ALL-AC-DIFF ≤ 8 × 10–5cm2/device at LET = 56.1MeV-cm2/mg, T = 25°C, 95% conf. and VDD = +5V, +5.5V
Run #(2) | Unit # | VDD (V) | Ion Type | LETEFF | Average Flux (× 103 ions-cm²/mg) | Fluence | Uniformity | #Events | Cross Section |
|---|---|---|---|---|---|---|---|---|---|
24 | 4 | 5 | Ag(109) | 56.1 | 10.30 | 1.99 | 95 | 98 | 49.2 |
25 | 4 | 5 | Ag(109) | 56.1 | 9.97 | 2.00 | 95 | 112 | 56.0 |
26 | 4 | 5.5 | Ag(109) | 56.1 | 9.87 | 2.01 | 94 | 104 | 51.7 |
27 | 4 | 5.5 | Kr(84) | 35.2 | 9.79 | 2.00 | 95 | 52 | 26.0 |
28 | 4 | 5 | Kr(84) | 35.2 | 9.88 | 2.00 | 94 | 49 | 24.5 |
29 | 4 | 5 | Kr(84) | 35.2 | 9.85 | 2.00 | 94 | 50 | 25.0 |
30 | 4 | 5 | Cu(63) | 24 | 10.20 | 2.00 | 92 | 30 | 15.0 |
31 | 4 | 5 | Cu(63) | 24 | 9.90 | 2.00 | 92 | 32 | 16.0 |
32 | 4 | 5.5 | Cu(63) | 24 | 9.21 | 2.00 | 95 | 34 | 17.0 |
33 | 4 | 5 | Ar(40) | 9.62 | 11.40 | 2.00 | 98 | 26 | 13.0 |
34 | 4 | 5 | Ar(40) | 9.62 | 11.40 | 2.00 | 98 | 25 | 12.5 |
35 | 4 | 5.5 | Ar(40) | 9.62 | 11.10 | 2.00 | 98 | 29 | 14.5 |
36 | 4 | 5 | Ne(20) | 3.01 | 17.10 | 2.00 | 96 | 10 | 5.0 |
37 | 4 | 5 | Ne(20) | 3.01 | 9.43 | 2.00 | 97 | 12 | 6.0 |
38 | 4 | 5.5 | Ne(20) | 3.01 | 9.22 | 2.00 | 96 | 11 | 5.5 |
42 | 4 | 5 | N(14) | 1.42 | 9.76 | 2.00 | 98 | 0 | 0.0 |
43 | 4 | 5 | N(14) | 1.42 | 9.96 | 2.00 | 99 | 0 | 0.0 |
44 | 4 | 5.5 | N(14) | 1.42 | 9.93 | 2.00 | 99 | 0 | 0.0 |
Figure 8-1 Cross Section and Weibull-Fit for DUT #4| Parameter | Value |
|---|---|
| Onset (MeV-cm2/mg) | 1.42 |
| σSAT (cm2) | 80 × 10–6 |
| W | 40 |
| s | 1 |
Figure 8-2 Worst Case Upset in AC Test When Monitoring Differential Output of the TRF0213-SEP