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. Author manuscript; available in PMC: 2017 Sep 9.
Published in final edited form as: Appl Opt. 2016 Jul 1;55(19):5208–5218. doi: 10.1364/AO.55.005208

Fig. 1.

Fig. 1

(a) Photograph of a released 4 mm diameter mirror with its four electrodes labeled. The resulting electrostatic force from the applied voltage is shown in the cross-section diagram. (b) Voltages resulting in the parabolic shape of the mirror allow for sharp imaging of infinite conjugate rays, while a non-parabolic shape leads to spherical aberration, where rays focus at different distances along the center axis. The total deflection, δ, represents the mirror sag of the reflective surface.