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061301_1_5.0148217.pdf
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Final Published Version
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Wyant College of Optical Sciences, University of ArizonaIssue Date
2023-06-16
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American Institute of Physics Inc.Citation
Maryam Baker, Euan McLeod; Lensfree time-gated photoluminescent imaging. APL Photonics 1 June 2023; 8 (6): 061301. https://doi.org/10.1063/5.0148217Journal
APL PhotonicsRights
© 2023 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution license.Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
Fluorescence and, more generally, photoluminescence enable high contrast imaging of targeted regions of interest through the use of photoluminescent probes with high specificity for different targets. Fluorescence can be used for rare cell imaging; however, this often requires a high space-bandwidth product: simultaneous high resolution and large field of view. With bulky traditional microscopes, high space-bandwidth product images require time-consuming mechanical scanning and stitching. Lensfree imaging can compactly and cost-effectively achieve a high space-bandwidth product in a single image through computational reconstruction of images from diffraction patterns recorded over the full field of view of standard image sensors. Many methods of lensfree photoluminescent imaging exist, where the excitation light is filtered before the image sensor, often by placing spectral filters between the sample and sensor. However, the sample-to-sensor distance is one of the limiting factors on resolution in lensfree systems and so more competitive performance can be obtained if this distance is reduced. Here, we show a time-gated lensfree photoluminescent imaging system that can achieve a resolution of 8.77 μm. We use europium chelate fluorophores because of their long lifetime (642 μs) and trigger camera exposure ∼50 μs after excitation. Because the excitation light is filtered temporally, there is no need for physical filters, enabling reduced sample-to-sensor distances and higher resolutions. © 2023 Author(s).Note
Open access journalISSN
2378-0967Version
Final Published Versionae974a485f413a2113503eed53cd6c53
10.1063/5.0148217
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Except where otherwise noted, this item's license is described as © 2023 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution license.

