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Complementary metal oxide semiconductor (CMOS) image sensor is susceptible to proton single event effect when being applied to space environment. Proton irradiation experiments with different energy values are carried out on a commercial FSI and BSI CMOS image sensors. The proton single event effect is analyzed by on-line testing, the maximum proton energy is 200 MeV, and the total fluence is 1010 particle/cm2. The single-event transient bright spots of different shapes are observed in the pixel array. By extracting the deposition energy and size, the effects of different energy protons on transient bright spot characteristics are compared, and the transient bright spot characteristics between FSI and BSI are also compared. Finally, the energy deposition distribution of the transient bright spot generated by proton in CMOS image sensor pixel unit is predicted by comparing the simulation method with the experimental results. The simulation results verify that the decrease of PPD depletion region thickness and the thinning of epitaxial layer are the main factors leading the proton energy deposition distribution to shift leftward in BSI image sensor.
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Keywords:
- CMOS image sensor /
- proton irradiation /
- single event effect /
- transient bright spot
[1] Sellier C, Gambart D, Perrot N, Garcia-Sanchez E, Virmontois C, Mouallem W, Bardoux A 2018 International Conference on Space Optics, Chania, Greece, 2018 11180
[2] BenMoussa A, Giordanengo B, Gissot S, et al. 2013 IEEE T. Electron. Dev. 60 1Google Scholar
[3] King E E, Nelson G P, Hughes H L 1972 IEEE T. Nucl. Sci. 19 264Google Scholar
[4] Ferlet C V, Dupont N E, Vildeuil J C 1998 Radecs 97: Fourth European Conference on Radiation and Its Effects on Components and Systems Paris, France, 1998
[5] Hancock B R, Soli G A 1997 IEEE T. Nucl. Sci. 44 1957Google Scholar
[6] Goiffon V, Estribeau M, Magnan P 2009 IEEE T. Electron. Dev. 56 2594Google Scholar
[7] Hopkinson G R, Mohammadzadeh A, Harboe-Sorensen R. 2004 IEEE T. Nucl. Sci. 51 2753Google Scholar
[8] Lalucaa V, Goiffon V, Magnan P 2013 IEEE T. Nucl. Sci. 60 2494Google Scholar
[9] Virmontois C, Toulemont A, Rolland G 2014 IEEE T. Nucl. Sci. 61 3331Google Scholar
[10] Cai Y L, Guo Q, Li Y D 2019 Solid-State Electronics 152 93
[11] Cai Y L, Wen L, Li Y D 2020 IEEE T. Nucl. Sci. 67 1861Google Scholar
[12] Beaumel M, Herve D, Van A D 2014 IEEE T. Nucl. Sci. 61 1909
[13] Hiemstra D M, Blackmore E W 2003 IEEE T. Nucl. Sci. 50 2245Google Scholar
[14] Warren K M 2010 Ph. D. Dissertation (Tennessee: Vanderbilt University)
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表 1 质子辐照信息
Table 1. Proton irradiation information.
能量/MeV LET/[MeV·(mg·cm–2)]–1 Si中射程/mm 样品数 60 8.6 × 10–3 16.8 1 100 5.9 × 10–3 41.6 1 150 4.4 × 10–3 84.6 1 200 3.6 × 10–3 138.6 1 -
[1] Sellier C, Gambart D, Perrot N, Garcia-Sanchez E, Virmontois C, Mouallem W, Bardoux A 2018 International Conference on Space Optics, Chania, Greece, 2018 11180
[2] BenMoussa A, Giordanengo B, Gissot S, et al. 2013 IEEE T. Electron. Dev. 60 1Google Scholar
[3] King E E, Nelson G P, Hughes H L 1972 IEEE T. Nucl. Sci. 19 264Google Scholar
[4] Ferlet C V, Dupont N E, Vildeuil J C 1998 Radecs 97: Fourth European Conference on Radiation and Its Effects on Components and Systems Paris, France, 1998
[5] Hancock B R, Soli G A 1997 IEEE T. Nucl. Sci. 44 1957Google Scholar
[6] Goiffon V, Estribeau M, Magnan P 2009 IEEE T. Electron. Dev. 56 2594Google Scholar
[7] Hopkinson G R, Mohammadzadeh A, Harboe-Sorensen R. 2004 IEEE T. Nucl. Sci. 51 2753Google Scholar
[8] Lalucaa V, Goiffon V, Magnan P 2013 IEEE T. Nucl. Sci. 60 2494Google Scholar
[9] Virmontois C, Toulemont A, Rolland G 2014 IEEE T. Nucl. Sci. 61 3331Google Scholar
[10] Cai Y L, Guo Q, Li Y D 2019 Solid-State Electronics 152 93
[11] Cai Y L, Wen L, Li Y D 2020 IEEE T. Nucl. Sci. 67 1861Google Scholar
[12] Beaumel M, Herve D, Van A D 2014 IEEE T. Nucl. Sci. 61 1909
[13] Hiemstra D M, Blackmore E W 2003 IEEE T. Nucl. Sci. 50 2245Google Scholar
[14] Warren K M 2010 Ph. D. Dissertation (Tennessee: Vanderbilt University)
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