Computational Imaging at the Infrared Beamline of the Australian Synchrotron Using the Lucy–Richardson–Rosen Algorithm
dc.contributor.author | Ng, Soon Hock | |
dc.contributor.author | Anand, Vijayakumar | |
dc.contributor.author | Han, Molong | |
dc.contributor.author | Smith, Daniel | |
dc.contributor.author | Maksimovic, Jovan | |
dc.contributor.author | Katkus, Tomas | |
dc.contributor.author | Klein, Annaleise | |
dc.contributor.author | Bambery, Keith | |
dc.contributor.author | Tobin, Mark J. | |
dc.contributor.author | Vongsvivut, Jitraporn | |
dc.contributor.author | Juodkazis, Saulius | |
dc.date.accessioned | 2024-04-04T12:47:49Z | |
dc.date.available | 2024-04-04T12:47:49Z | |
dc.date.issued | 2023 | |
dc.description.abstract | The Fourier transform infrared microspectroscopy (FTIRm) system of the Australian Synchrotron has a unique optical configuration with a peculiar beam profile consisting of two parallel lines. The beam is tightly focused using a 36× Schwarzschild objective to a point on the sample and the sample is scanned pixel by pixel to record an image of a single plane using a single pixel mercury cadmium telluride detector. A computational stitching procedure is used to obtain a 2D image of the sample. However, if the imaging condition is not satisfied, then the recorded object’s information is distorted. Unlike commonly observed blurring, the case with a Schwarzschild objective is unique, with a donut like intensity distribution with three distinct lobes. Consequently, commonly used deblurring methods are not efficient for image reconstruction. In this study, we have applied a recently developed computational reconstruction method called the Lucy–Richardson–Rosen algorithm (LRRA) in the online FTIRm system for the first time. The method involves two steps: training step and imaging step. In the training step, the point spread function (PSF) library is recorded by temporal summation of intensity patterns obtained by scanning the pinhole in the x-y directions across the path of the beam using the single pixel detector along the z direction. In the imaging step, the process is repeated for a complicated object along only a single plane. This new technique is named coded aperture scanning holography. Different types of samples, such as two pinholes; a number 3 USAF object; a cross shaped object on a barium fluoride substrate; and a silk sample are used for the demonstration of both image recovery and 3D imaging applications. | |
dc.identifier.uri | https://doi.org/10.3390/app132312948 | |
dc.identifier.uri | https://hdl.handle.net/10062/97770 | |
dc.language.iso | en | |
dc.relation | info:eu-repo/grantAgreement/EC/H2020/857627///CIPHR | |
dc.rights | Attribution-NonCommercial-NoDerivs 3.0 Estonia | en |
dc.rights.uri | http://creativecommons.org/licenses/by-nc-nd/3.0/ee/ | |
dc.subject | computational imaging | |
dc.subject | holography | |
dc.subject | Lucy–Richardson–Rosen algorithm | |
dc.subject | microscopy | |
dc.subject | spectroscopy | |
dc.subject | image processing | |
dc.subject | non-linear reconstruction | |
dc.subject | Lucy–Richardson algorithm | |
dc.subject | mid-infrared imaging | |
dc.subject | Fourier transform infrared microspectroscopy | |
dc.title | Computational Imaging at the Infrared Beamline of the Australian Synchrotron Using the Lucy–Richardson–Rosen Algorithm | |
dc.type | info:eu-repo/semantics/article | en |
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