Chinese Optics, Volume. 18, Issue 2, 256(2025)
Damage mechanism of back-illuminated CMOS image sensor irradiated by pulsed laser
Fig. 1. The two-dimensional structure of the back-illuminated CMOS image sensor
Fig. 2. Radiation results of 532 nm nanosecond single pulse laser. (a) Temperature distribution; (b) maximum temperature change in each layer
Fig. 3. Radiation results of
Fig. 4. Radiation results of 532 nm picosecond single pulse laser. (a) Temperature distribution; (b) maximum temperature change in each layer
Fig. 5. Radiation results of
Fig. 6. Experimental block of CMOS image sensor irradiated with 532 nm nanosecond single pulse laser
Fig. 7. Light path of CMOS image sensors irradiated by 532 nm nanosecond single pulse laser
Fig. 8. Damage condition of CMOS image sensors irradiated by 532 nm nanosecond single pulse laser. From left to right, the laser energy densities are 28.95 mJ/cm2, 69.91 mJ/cm2, 167.6 mJ/cm2, 519.3 mJ/cm2, respectively
Fig. 9. Experimental principle of CMOS image sensor irradiated with
Fig. 10. Light path of CMOS image sensor irradiated with
Fig. 11. Damage condition of CMOS image sensors irradiated by
Fig. 12. Experimental principle of CMOS image sensor irradiated with picosecond single pulse laser
Fig. 13. Light path of CMOS image sensor irradiated with single pulse picosecond laser
Fig. 14. Damage condition of CMOS image sensor irradiated by 532 nm picosecond pulse laser. From left to right, the laser energy densities are 18.95 mJ/cm2, 78.93 mJ/cm2, 120.49 mJ/cm2, 501.33 mJ/cm2, respectively
Fig. 15. Damage condition of CMOS image sensor irradicatd by
Fig. 16. Comparison between simulation results and experimental results of point damage threshold
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Fang QIAN, Jia-qi PENG, Yong-bo XU. Damage mechanism of back-illuminated CMOS image sensor irradiated by pulsed laser[J]. Chinese Optics, 2025, 18(2): 256
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Received: Aug. 1, 2024
Accepted: Oct. 22, 2024
Published Online: May. 19, 2025
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