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Imprint lithography is a promising technology for replication of nano-scale features. For semiconductor device applications, Canon deposits a low viscosity resist on a field by field basis using jetting technology. A patterned mask is lowered into the resist fluid, which then quickly flows into the relief patterns in the mask by capillary action. Following this filling step, the resist is crosslinked under UV radiation, and then the mask is removed, leaving a patterned resist on the substrate. Overlay budgets play a large role in defining production readiness. As an example, DRAM devices require overlay on the order of 15-20% of the half pitch. Canon uses a through the mask (TTM) alignment system to measure a Moiré image anywhere in the field. This system can also record alignment errors of all fields and all marks. The data collected by the TTM system correlates very closely with an Archer measurement tool. In addition, a High Order Distortion Correction (HODC) system, which applies a heat input on a field by field basis through the use of a DMD array has been combined with magnification actuators to correct high order distortion terms up to K30. There is an additional distortion term that must also be addressed for the case of nanoimprint lithography. NIL drop patterns are typically designed to minimize resist fill time and create a uniform residual layer beneath the resist pattern. For device wafers, however, it is important to recognize that there are both long wavelength flatness errors coming from the wafer chuck and existing pattern topography from previously patterned levels that cause out of plane errors. When the mask comes in contact with the resist on the wafer, these out of plane errors can then induce mask bending, resulting in an additional distortion term. To minimize this distortion, a Drop Pattern Compensation (DPC) Model has been implemented to minimize the added distortion terms. In this paper we present an updated study and report on nanoimprint mix and match overlay improvements using DPC. In addition, we describe how the mode array and peak to valley thickness of the resist impacts distortion correction.
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