Bulletin of the American Physical Society
2018 Annual Meeting of the APS Four Corners Section
Volume 63, Number 16
Friday–Saturday, October 12–13, 2018; University of Utah, Salt Lake City, Utah
Session C05: AMO1: Optical Measurement |
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Chair: Arvinder Sandhu, University of Arizona Room: CSC 208 |
Friday, October 12, 2018 10:45AM - 11:09AM |
C05.00001: Taking High Resolution Images with a Lensless, Single Pixel Camera Invited Speaker: Dallin S. Durfee Structured illumination imaging is a method of capturing an image without the need for an imaging lens or a multi-pixel detector. By projecting known patterns of light onto an object, and measuring how much light the object scatters, information about the object can be collected, and then processed into an image. In our lab we are using laser interference to generate structured illumination patterns. This technique has some significant advantages over previous work, including the ability to achieve microscopic resolution with no optics near the object imaged, a depth of field and field of view which are independent of the resolution, and the ability to surpass the resolution limit of conventional imaging without any expensive high numerical aperture optic. And because the technique doesn't require a precise lens or multi-pixel detector, it could easily be applied to imaging with x-rays, radar waves, acoustic waves, or other waves for which these elements are difficult to manufacture. |
Friday, October 12, 2018 11:09AM - 11:21AM |
C05.00002: Construction and Characterization of an Avalanche Photodiode Detector Benjamin G. Whetten, Jarom S. Jackson, Dallin S. Durfee Traditional photodetectors built using photodiodes are relatively inexpensive, robust, and have high quantum efficiencies, but their responsivity is small. Photomultiplier tubes have much higher responsivities due to electron avalanche multiplication, but have lower quantum efficiency, are more expensive, and fragile. Avalanche photodiodes have many of the advantages of standard photodiodes, but also utilize electron avalanche multiplication. We are working on constructing a small, precise, and inexpensive avalanche photodiode detector utilizing modern voltage converter and amplifier chips. This detector would use a commercially available avalanche photodiode instead of a regular photodiode to achieve a higher internal gain while maintaining a large quantum efficiency to allow more accurate measurements of low intensity light. |
Friday, October 12, 2018 11:21AM - 11:33AM |
C05.00003: Optical Characterization of Zinc Oxide Thin Film Semiconductors James W Erikson, John S Colton Zinc oxide is a wide band gap semiconductor with many potential applications, including ultraviolet lasers, transparent circuits, and radiation resistant devices. In order to create these devices, both n- and p- type materials are required, however reliable methods of p-type doping of zinc oxide have yet to be developed. We have attempted to grow arsenic doped zinc oxide films using RF magnetron sputtering. Sample quality and doping are studied with stimulated photoluminescence, which has been found to improve with As doping and annealing processes. This in turn allows us to further refine our film growth process in the hopes of creating consistently p-type material. |
Friday, October 12, 2018 11:33AM - 11:45AM |
C05.00004: Effect of Scaling on the Optical Q of SiN Optomechanical Oscillators Amy Lili Soudachanh, Alejandro Grine, Darwin K Serkland, Michael Wood, Christopher Hains, Andrew Hollowell, Lawrence Koch, Katherine M Musick, Lidia Ruiz, Jay Bischoff Cavity optomechanical oscillators (OMOs) have several applications in timing, communications and sensors. For all applications, it is interesting to investigate the effect of reduced device size on optical quality factor, Q. In this study, we measure the optical Q at 1550 nm of released SiN whispering gallery mode resonator OMOs coupled to SiN waveguides. We chose a free space optical setup for flexible mode matching and long-term stability. The setup takes advantage of a top down camera and co-linear, co-focused 635 nm and 1550 nm lasers for easier waveguide coupling. We also describe improvements in automation for real time resonance identification and analysis. The devices measured are discs and anchored ring resonators with varying waveguide coupling gaps and device radii ranging from 10 μm to 60 μm which are suspended with various spoke widths. We achieved Q=2x106 in 50 μm radius discs. A comparison of optical Q as a function of the parameters stated above will be made to determine designs for optomechanical characterization. |
Friday, October 12, 2018 11:45AM - 11:57AM |
C05.00005: Optical Transmission of Radiated Optical Filters Ashlan Keeler, JR Dennison, John Stauder, Brian D Wood, Jonh Carlos Mojica Decena The effects of ionizing beta radiation on the UV/VIS/NIR optical transmission of coated optical filters was studied. Three coated optical elements were irradiated, a wide-band pass filter and two short pass filters. The transmission for the two short pass filters decreased with dose, but increased for the wide-band pass filter. The optical transmission is expected to change linearly with total ionizing dose. Radiation creates additional localized defect sites in the coating materials, increasing the absorptivity of the coatings. This readily explains the behavior of single layer absorptive short pass filters. By contrast the differential change in absorptivity of different layers of the multilayer dichroic band pass filter can affect constructive or destructive interference effects which are responsible for the band pass, by altering the intensity of the constituted reflected rays from each subsequent layer’s interface. Thus, increased absorption can, at least qualitatively, explain the increased transmission of the band pass filter. Bombarded by radiation from the sun and extra-solar sources and radiation belts, this research helps understand how optical filters change in space. |
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