Figure 7 Dynamic range expansion of Shack- Hartmann sensor using a spatial-light modulator

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Figure 4 Advantage of having smaller focal spot on CCD with super-fine pixels: Larger focal point compromises the sensitivity, spatial resolution, and accuracy. Figure 1 Typical microlens array for Shack-Hartmann Sensor (S: Pitch between neighboring microlenses, G L : Gap between neighboring microlenses, D L : Diameter of microlenses, Numbers in blue: Identification numbers assigned to microlenses) Figure 5 Dislocation of focal points due to large curvature of the wavefront: The focal points of microlens #1 and #3 are dislocated onto the subapertures assigned to microlens #4 and #5, respectively, causing erroneous measurements. Figure 2 Wavefront slope measurement using microlens array: Each microlens has its own subaperture consisted of four CCD pixels, and the focal point of the microlens must be located within the assigned sub-aperture. Figure 6 Dynamic range expansion using astigmatic microlenses and its failure: Once the focal point becomes circular, its origin cannot be traced. Figure 3 Advantage of having smaller pixels: CCD with larger pixels (left) cannot detect the shift in position of the focal spot while CCD with smaller pixels (right) can easily detect the change. Figure 7 Dynamic range expansion of Shack- Hartmann sensor using a spatial-light modulator

1. Spin-coat a.2 µm thick Teflon (hydrophobic) layer on quartz wafer. Then, photolithographically pattern and dry-etch the Teflon layer using low power O 2 plasma. 2. Using the inkjet print head, dispense the desired amount of UV-curable polymer within the hydrophilic circles. 3. Fully cure the polymer lens under a high-intensity UV lamp. Figure 8 Fabrication Process: Printer Microlens (Smaller Volume) Diameter =D Stroboscopic View of Droplet Quartz Substrate Teflon Figure 9 Various hydrophilic patterns created on a hydrophobic Teflon layer on quartz substrate Printer Microlens (Larger Volume) Stroboscopic View of Droplet Diameter =D Figure 11 Controlling the curvature of 1 µmdiameter microlens: Change in volume clearly changes the curvature/height of the microlens for a given diameter. Figure 1(a) Fabrication setup: printer and driver, automated stage, and viewing system. Figure 12 Uniform 4 µm-diameter microlenses Figure 1(b) Enlarged view of microjet printer, automated stage, and viewing system Figure 13 Variation of microlens curvatures for 4- µm diameter

Effective Focal Length 8 7 6 5 4 3 2 1 Effective Focal Length Vs Microlens Volume 2 micron Diameter 4 micron Diameter 6 micron Diameter 1 micron Diameter 5 1 15 2 25 3 35 Microlens Volume (pico liter) Figure 14 Effective focal length Vs microlens volume.5.25 (in micron).15.1.5 (in micron).15.1.5 Vs Effective Focal Length for 2 micron-diameter Microlenses Aperture: 9% of Microlens Diameter Aperture: 5% of Microlens Diameter 25 3 35 4 45 Effective Focal Length Vs Effective Focal Length for 4 micron-diameter Microlenses Aperture: 9% of Microlens Diameter Aperture: 5% of Microlens Diameter Aperture: 3% of Microlens Diameter 5 1 15 2 25 Effective Focal Lengths (in micron) Vs Effective Focal Length for 6 micron-diameter Microlenses Aperture: 9% of Microlens Diameter Aperture: 5% of Microlens Diameter Aperture: 3% of Microlens Diameter 18 23 28 33 38 Effective Focal Length (in micron).15.1.5 Vs Effective Focal Length for 1 micron-diameter Microlenses Aperture: 9% of Microlens Diameter Aperture: 5% of Microlens Diameter Aperture: 3% of Microlens Diameter 27 37 47 57 67 77 Effective Focal Length Figure 15 Rms wavefront error Vs effective focal length for various microlenses Figure 16 Producing a master element for highprecision microlens replication 417-nm licon Nitride licon Nitride licon Nitride 4.25 mm 5 mm Figure 17 Beam splitter process flow a) LPCVD low-stress silicon nitride on substrate. Etch back with 16 C phosphoric acid, for 417-nm membrane thickness. b) Pattern and DRIE etch back-side silicon nitride. c) KOH back-side etch forming suspended membrane. Figure 18 ngle-, double-, triple-nitride membrane

Frame Nitride Mirror Rotating Hinge Bimorph Hinge Figure 19 Possible integration schemes for the multilayer with MEMS structures Figure 21 Schematic diagram of active MEMS microlens array and enlarged view of individually active microlens unit 635-nm Laser Diode Commercial Cubic Collimating Lens Thin Film Figure 22 Actual layout of our prototype active MEMS microlens array and enlarged view of individually active microlens unit Photo Intensity Detector Mirror Figure 2 Optical testing setup for thin-film 1. RIE the device layer to create an opening for microlens. 2. Deposit LPCVD low stress nitride layer. 3. Pattern the nitride layer and RIE the device layer to create MEMS actuators. 4.RIE the handling layer to create an opening for microlens. 5. Release the structure in 49% concentrated HF. 6. Make microlens using our Polymer-Jet printer. Figure 23 Fabrication Process for active MEMS microlens array:

Table 1 Reflected and transmitted light extinction ratios for single-, double-, and triple-nitride membranes ngle- Double- Triple- Layer Layer Layer * Stacked Stacked Insertion Loss 3% 1% 13% Reflected 99.2% 99.2% 99.2% /Reflected Transmitted 9.9% 96.2% 97.5% /Transmitted Reflected Light Extinction Ratio (db) Transmitted Light Extinction Ratio (db) Layer 1 (nm) Layer 2 (nm) Layer 3 (nm) 21 21 21 1 14 16 419.3 419.5 419.5 N/A 419.2 419.2 N/A N/A 419.5 * Average values for 1 different single-layer structures