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. 2021 May 25;7:39. doi: 10.1038/s41378-021-00266-x

Fig. 3. Latent image simulations of varying photomask occulter diameters and air gaps.

Fig. 3

The ordinate is the top downwards photoresist thickness, T, (µm), and the abscissa is the feature diameter, D, (µm). The unobstructed aerial ED = 1700 mJ/cm2, diffraction λ=405 nm and the simulation resolution is 0.5 µm for (ad) and 1 µm for (ep). The figure color scales with photoresist thickness to differentiate between height levels, where colored data points represent sites of cross-linked photoresist. Rows 1–4 correspond to 10, 20, 50, and 100 µm diameter circular occulters, respectively. Columns 1–2 and 3–4 correspond to air gaps of 1 and 100 µm. a 2D x-z photoresist cross-section with D=10 µm and g=1 µm. Light intensity calculation time (t) = 2 s. b 3D wrap-around view of (a) with a z-axis of rotation at x=0 and y=0. c 2D cross-section with D=10 µm, g=100 µm and t = 1 s. d 3D wrap-around view of (c). e 2D cross-section with D=20 µm, g=1 µm and t = 5 s. f 3D wrap-around view of (e). g 2D cross-section with D=20 µm, g=100 µm and t = 1 s. h 3D wrap-around view of (g). i 2D cross-section with D=50 µm, g=1 µm and t = 37 s. j 3D wrap-around view of (i). k 2D cross-section with D=50 µm, g=100 µm and t = 15 s. l 3D wrap-around view of (k). m 2D cross-section with D=100 µm, g=1 µm and t = 1 m 41 s. n 3D wrap-around view (m). o 2D cross-section with D=100 µm, g=100 µm and t = 1 m 1 s. p 3D wrap-around view of (o)