2006
DOI: 10.1117/12.655904
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OPC and PSM design using inverse lithography: a nonlinear optimization approach

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Cited by 51 publications
(60 citation statements)
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“…where J 1 is the Bessel function of the first kind, order one [22], NA is the numerical aperture of the projection lens, and λ is the source light wavelength. 2) Once the optical image falls on the photoresist-coated wafer, the photoresist is developed and etched based on image intensity at the corresponding wafer location.…”
Section: ) Illumination Modulementioning
confidence: 99%
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“…where J 1 is the Bessel function of the first kind, order one [22], NA is the numerical aperture of the projection lens, and λ is the source light wavelength. 2) Once the optical image falls on the photoresist-coated wafer, the photoresist is developed and etched based on image intensity at the corresponding wafer location.…”
Section: ) Illumination Modulementioning
confidence: 99%
“…If the photoresist material is positive (negative) and the image intensity at a certain location is greater (lesser) than a specific threshold, the resist gets etched out. The resulting image is called the resist or pattern image I and is often calculated as follows [22]:…”
Section: ) Illumination Modulementioning
confidence: 99%
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“…Hence, there has recently been a revival of interest in pixel-based ILT approaches. [4][5][6][7] In this work, we extend our earlier proposed singleexposure ILT framework 7 to double-exposure lithography ͑DEL͒ systems. Double-exposure lithography has gained a lot of importance recently and is tipped as one of the important technologies for enabling 45 nm and smaller technology nodes.…”
Section: Introductionmentioning
confidence: 99%