Gustavo Espinel

Multiple-Bit Upset in 130 nm CMOS Technology

The probability of proton-induced multiple-bit upset (MBU) has increased in highly-scaled technologies because device dimensions are small relative to particle event track size. Both proton-induced single event upset (SEU) and MBU responses have been shown to vary with angle and energy for certain technologies. This work analyzes SEU and MBU in a 130 nm CMOS SRAM in which the single-event response shows a strong dependence on the angle of proton incidence. Current proton testing methods do not account for device orientation relative to the proton beam and, subsequently, error rate prediction assumes no angular dependencies. Proton-induced MBU is expected to increase as integrated circuits continue to scale into the deep sub-micron regime. Consequently, the application of current testing methods will lead to an incorrect prediction of error rates

The Effects of Irradiation Temperature on the Proton Response of SiGe HBTs

We compare, for the first time, the effects of 63 MeV protons on 1st generation and 3rd generation SiGe HBTs irradiated at both liquid nitrogen temperature (77 K) and at room temperature (300 K). The 1st generation SiGe HBTs irradiated at 77 K show less degradation than when irradiated at 300 K. Conversely, the 3rd generation SiGe HBTs exhibits an opposite trend, and the devices irradiated at 77 K show enhanced degradation compared to those irradiated at 300 K. The emitter-base spacer regions for these two SiGe technologies are fundamentally different in construction, and apparently are responsible for the observed differences in temperature-dependent radiation response. At practical circuit biases, both SiGe technology generations show only minimal degradation for both at 77 K and 300 K exposure, to Mrad dose levels, and are thus potentially useful for electronics applications requiring simultaneous cryogenic temperature operation and significant total dose radiation exposure

Substrate Engineering Concepts to Mitigate Charge Collection in Deep Trench Isolation Technologies

Delayed charge collection from ionizing events outside the deep trench can increase the SEU cross section in deep trench isolation technologies. Microbeam test data and device simulations demonstrate how this adverse effect can be mitigated through substrate engineering techniques. The addition of a heavily doped p-type charge-blocking buried layer in the substrate can reduce the delayed charge collection from events that occur outside the deep trench isolation by almost an order of magnitude, implying an approximately comparable reduction in the SEU cross section

Proton Tolerance of SiGe Precision Voltage References for Extreme Temperature Range Electronics

A comprehensive investigation of the effects of proton irradiation on the performance of SiGe BiCMOS precision voltage references intended for extreme environment operational conditions is presented. The voltage reference circuits were designed in two distinct SiGe BiCMOS technology platforms (first generation (50 GHz) and third generation (200 GHz)) in order to investigate the effect of technology scaling. The circuits were irradiated at both room temperature and at 77 K. Measurement results from the experiments indicate that the proton-induced changes in the SiGe bandgap references are minor, even down to cryogenic temperatures, clearly good news for the potential application of SiGe mixed-signal circuits in emerging extreme environments

Single Event Upset Mechanisms for Low-Energy-Deposition Events in SiGe HBTs

Microbeam measurements and TCAD simulations are used to examine the effects of ion angle of incidence on the charge collected from events occurring in a Silicon Germanium (SiGe) Heterojunction Bipolar Transistor (HBT). The results identify the geometrically driven charge-collection mechanisms that dominate the low LET broad beam SEU response. The deep trench isolation that surrounds the transistor significantly modulates the charge transport and, therefore, the charge collected by the collector. A new way of estimating critical charge, , for upset in SiGe HBT circuits is proposed based on TCAD simulation results and measured broadbeam data.

CMOS Device Reliability for Emerging Cryogenic Space Electronics Applications

0C (43K) in the polar shadows), makes operation of the electronics sub-systems on the surface of the Moon exceptionally difficult, but is nonetheless required for the envisioned complex suite of electronics systems used in sensing, actuation, and control of robotic systems. Such applications are typically fairly low frequency in nature (e.g., < 100 MHz), hence not requiring the most aggressively scaled CMOS technology; however, a full suite of mixed-signal circuit building blocks, and reliable operation of those circuits across extremely large variations in temperature (e.g., +120 to -230C) is needed. Adequate device reliability must clearly be achieved to accomplish this task. CMOS device degradation due to hot carriers effect (HCE) is known to be considerably worse at low temperatures [2]. Device lifetime data at cryogenic temperatures, and a solid understanding of the corresponding degradation mechanisms, are thus critical in this context of space electronics, and are addressed in this work. The Si CMOS devices investigated here are from an advanced 0.5µm SiGe BiCMOS technology, with a fixed channel width of 10.0 µm, and effective gate lengths ranging from 0.35 µm (minimum geometry), to 5.0 µm. The devices were characterized on a custom cryogenic probe system from 300K down to 43 K (-230 0 C). For brevity we will focus on the nFET data, since it represents the worst case in this technology. Fig. 1 and 2 shows typical I-V characteristics for the CMOS devices at different temperatures. The current drive capability increases significantly for the same bias conditions, as the temperature decreases. The nFET lifetime was inferred using stress-induced changes to the ID-VG characteristics. The lifetime τ is defined here as the inferred stress time for which a certain parameter of the ID-VG characteristics has shifted by a predefined amount (e.g., 10% degradation of gm). A typical lifetime assessment analysis using the ID-VG characteristics for a 1.0 µm nFET are shown in Fig. 3 and Fig. 4. The slope of 0.6 for the linear fitting in Fig. 4 suggests that interface state generation is responsible for the observed device degradation at the maximum substrate current (VG ≈ ½ VD); while that of 0.3 for the maximum gate current bias condition (VG = VD) suggests that oxide trapped charge dominates [3]. For the nFETs operating at 300K, the worst case bias condition for hot carrier degradation is known to be under maximum substrate current bias. There has been speculation that the worst case bias conditions for hot carrier degradation can, however, be a function of temperature [4]. It can be verified from Fig. 4 that for this technology, maximum substrate current is indeed the worst bias condition, at least down to 82K, and hence was the condition used here for device lifetime evaluation. The substrate current is comprised of the generated hot carriers, and is thus a good monitoring parameter for HCE in practical measurements. Fig. 5 and Fig. 6 show the effects of temperature and gate length on substrate current, respectively. It can be seen from Fig. 5 that the maximum substrate current under the same bias condition increases by 3x as temperature decreases from 300K to 43K; while Fig. 6 suggests that the maximum substrate current increases by more than 10x as L shrinks from 1.0 µm to 0.35 µm, and becomes negligible as L increases to 5.0 µm. This suggests that HCE is impacted more by device geometry than by the temperature. Fig. 7 shows the inferred lifetime at different drain bias’ at different temperatures. As seen in Fig. 7, τ decreases by ~10x as the temperature is reduced from 300K to 82K. Furthermore, τ differs by more than 100x between the 1.0 µm and 0.35/5 µm transistors, and hence the longer-channel devices are preferred for cryogenic applications of this technology Assuming fast interface trap generation dominates the HCE degradation, plotting τID versus ISUB/ID on a log-log scale should yield a straight line behavior [5]. The critical electron energy for generating an interface trap is calculated to be 3.9 eV from the slop of the line. Both the slope and the critical energy from Fig. 8 correlate well with literature data (2.9 and 3.7 eV in [5]), suggesting that interface state generation is the dominant limiting reliability factor at low temperatures.