SBAA222A October   2017  – April 2025 ADS1282-SP

 

  1.   1
  2.   Abstract
  3.   Trademarks
  4. Overview
  5. SEE Mechanisms
  6. Test Device and Evaluation Board
  7. Irradiation Facility and Setup
    1. 4.1 Depth, Range, and LETeff Calculation
  8. Test Setup and Procedures
    1. 5.1 SEE Testing Block Diagram
    2. 5.2 Test Parameters
    3. 5.3 Test Conditions
  9. SET Test Results
  10. SEL Test Results
  11. Conclusions
  12. Acknowledgment
  13. 10References
  14. 11Revision History

Depth, Range, and LETeff Calculation

The ADS1282-SP is fabricated in the Texas Instruments high-performance analog 130-nm BiCMOS process (HPA07) with a back-end-of-line (BEOL) stack consisting of X levels of standard thickness aluminum metal on a Y-µm pitch, and a fourth level of thick aluminum. The total stack height from the surface of the passivation to the silicon surface is 10µm, based on nominal layer thickness as shown in Figure 4-2. No polyimide or other coating was present so the uppermost layer was the nitride passivation layer (PON). Accounting for energy loss through the 1-mil thick Aramica (Kevlar®) beam port window, the 40mm air gap, and the BEOL stack over the ADS1282-SP, the effective LET (LETeff) at the surface of the substrate and the depth and ion range was determined with the custom RADsim-IONS application (custom tool developed at Texas Instruments based on SRIM 2013 [9]) simulations for the two primary ions used for the experiments. The results are shown in Table 4-1. The stack was modeled as a homogeneous layer of silicon dioxide.

 HPA07
                        Technology BEOL Stack Cross-Section on the ADS1282-SPFigure 4-2 HPA07 Technology BEOL Stack Cross-Section on the ADS1282-SP
 RADsim-IONS Application GUIFigure 4-3 RADsim-IONS Application GUI

Generalized cross-section (left) of the HPA07 technology BEOL stack on the ADS1282-SP. GUI of RADsim-IONS application (right) used to determine key ion parameters: LETeff, depth, and range for a given ion type, energy, and stack. LETeff has been adjusted to account for beam degraders inserted into the beam line.

Table 4-1 Ions and Angles Used in SEE Experiments
ION TYPE ANGLE OF INCIDENCE DEPTH IN SILICON (µm) RANGE IN SILICON (µm) LETeff (MeV × cm2/ mg)
Ne 250.1 250.1 2.7
Ar 169.5 169.5 8.4
Kr 106.8 106.8 28.3
Ag 87.8 87.8 42.8
Ag 32° 72.9 86.0 50.5
Xe 82.4 82.4 52.3
Xe 30° 70.0 80.8 60.4