Abstract

Adaptive optical (AO) components play an important role in numerous optical applications, from astronomical telescopes to microscope imaging systems. For most of these AO components, the induced wavefront correction, respectively added optical power, is based on a rotationally symmetric or segmented design of the AO component. In this work, we report on the design, fabrication, and characterization of a micro-electronic-mechanical system (MEMS) adaptive membrane mirror in the shape of a parabolic cylinder. In order to interpret the experimental characterization results correctly and provide a tool for future application development, this is accompanied by the setup of an optical simulation model. The characterization results showed a parabolically deformable membrane mirror with an aperture of 8 × 2 mm2 and an adaptive range for the optical power from 0.3 to 6.1 m−1 (dpt). The optical simulation model, using the Gaussian beamlet propagation method, was successfully validated by laser beam profile measurements taken in the optical characterization setup. This MEMS-based adaptive astigmatic membrane mirror, together with the accompanying simulation model, could be a key component for the rapid development of new optical systems, e.g., adaptive laser line generators.

Highlights

  • An increasing number of optical systems utilize adaptive optical (AO) components, which allow for an electronically controlled variation of the optical key parameters

  • We present and characterize a novel AO component, a micro-electronic-mechanical system (MEMS)-based adaptive astigmatic membrane (MAAM) mirror

  • Because we aimed to develop a general simulation model for laser applications of the MAAM mirror, Gaussian beamlet propagation (GBP) was chosen due to its ability to represent coherent beams in astigmatic beam configurations

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Summary

Introduction

An increasing number of optical systems utilize adaptive optical (AO) components, which allow for an electronically controlled variation of the optical key parameters. These components range from surface curvature-changing liquid-filled membrane devices up to micro-electronic-mechanical system (MEMS)-based deformable mirrors [1,2]. For these systems, a widespread range of optical applications can be found. The induced deformation in the AO component typically can lead to a wavefront correction in the range of 10 to 20 waves (about 5–10 μm)

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