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Figure 1
(A) Light transmission of different viscous jetting materials measured in flat cells of 22, 100, 200 and 500 µm path lengths using an integration sphere detector and fitted with the Kubelka–Munk model. (B) Exemplary forward light flux I(x) and backward light flux J(x) simulated for a 150 µm-thick sample layer using the Kubelka–Munk theory. |
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