15 research outputs found

    Optimum performance allowable by a goggle lens correction: On-axis optical quality gain OQG of various liquid lenses via corneal index matching optical correction.

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    <p>The stairs function corresponds to the alternative solution of a ‘non-corneal matching index’ with a 2-element air-spaced goggle lens. The performance by indirect optical correction at various pupil diameters appears on the upper axis.</p

    Visualization 1: Three-dimensional photoacoustic imaging via scanning a one dimensional linear unfocused ultrasound array

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    animation for two carbon phantom Originally published in Optics Express on 03 April 2017 (oe-25-7-8022

    Robustness to lens fitting errors: Wide-angle resolution achieved for a 2-mm pupil diameter over a +/-10 degree field angles using a tunable artificial cornea alone (red symbols) and in combination with a conjugated adaptive plano-element (blue symbols) conjugated to the pupil of the eye, as a function of a) decentering and b) tilting of the goggle lens with respect to the eye pupil.

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    <p>The black and blue dashed baselines indicate the performance achieved using a single AO corrector conjugated to the eye pupil and the cornea, respectively. Below those 2 baselines, the performance of an adaptive correction using a single plano-element dominates an artificial cornea correction. Note that association of AO with an artificial cornea brings an outstanding performance benefit for wide-angle images, as compared to an artificial cornea alone and a single AO corrector alone.</p

    Media 2: High-resolution dual-modality photoacoustic ocular imaging

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    Originally published in Optics Letters on 15 April 2014 (ol-39-8-2451

    Media 1: High-resolution dual-modality photoacoustic ocular imaging

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    Originally published in Optics Letters on 15 April 2014 (ol-39-8-2451

    Confocal, corresponding CW-STED, and deconvolved STED images of keratin intermediate filaments in a PtK2 cell stained with ATTO 647N.

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    <p>(a) Confocal; (b) CW-STED; (c) R-L deconvolution of (b). The intensity at the cross-section marked in (a), (b), and (c) boxed regions are plotted in (d). The wavelength and power density for STED beam is 763 nm and ∼200 MW/cm<sup>2</sup>. Scale bar: 1 µm.</p
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