Journal
APPLIED OPTICS
Volume 44, Issue 20, Pages 4228-4238Publisher
OPTICAL SOC AMER
DOI: 10.1364/AO.44.004228
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In the classical Hartmann test the wave front is obtained by integration of the transverse aberrations, joining the sampled points by small straight segments, in the so-called Newton integration. This integration is performed along straight lines joining the holes on the Hartmann screen. We propose a modification of this procedure, considering the cells of four holes of the Hartmann screen to fit a small second-power wave front recovering each square. This procedure has some important advantages, as described here. (c) 2005 Optical Society of America.
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