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    <datestamp>2024-10-17T16:39:38Z</datestamp>
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<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:date>2024-10-17</dc:date>
  <dc:title>Data of Research on optimization method of underwater scattering imaging based on off-axis digital holography</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.14484</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>This folder contains manuscript titled &amp;quot;Research on optimization method of underwater scattering imaging based on off-axis digital holography&amp;quot; and the detailed 20 figures of this project.Fig.1.Underwater off-axis digital hologram imagingFig.2.Flow chart of hologram reconstructionFig.3 4F system filtering schematic diagramFig.4 Simulation target and scattering medium. ( a ) Target image ; ( b ) Scattering mediaFig.5 Direct imaging and holographic imaging. (a) Direct imaging; (b) Hologram; (c) Reconstruction mapFig.6 Holographic imaging with or without 4F system. (a)holograms without 4F;(b) holograms with 4F; (c)reconstruction image without 4F ;(d) reconstruction image with 4F.Fig.7 Comparative analysis of hologram reconstruction effect under different light intensity. (a) 10&amp;times;;(b) 100&amp;times;；(c) 1000&amp;times;;(d) 10000&amp;times;.Fig.8 Three-dimensional sketch of Butterworth FilterFig.9 Three-dimensional schematic of the filter. ( a ) Ideal low-pass filter ( b ) Gaussian low-pass filterFig.10 Different filter reconstruction of the same hologram. (a) Ideal filter ; (b) Gaussian filter (c) Butterworth filterFig11.Underwater off-axis digital holographic imaging experimental setup based on 4F systemFig12 Imaging results of direct imaging and holographic imaging at different attenuation lengths(a)~(d) are the results of direct imaging.Fig13.The imaging results of holographic imaging with or without 4F system at different attenuation lengths.(a)~(d) are holograms without 4F system imaging. (e)~(f) are holograms with 4F system imaging.Fig14.The reconstruction results of holograms with or without 4F system holographic imaging system at different attenuation lengths. (a)~ (d) are the reconstruction of hologram without 4F system. &amp;nbsp;(e)~(f) are the reconstruction of hologram with 4F system.Fig.15 Holographic reconstruction images with different attenuations at different light intensity ratios. &amp;nbsp;&amp;nbsp;(a)10x；(b)50x；(c)100x；(d)500xFig.16 Comparison of holographic reconstruction images with different attenuations at different reference light intensity ratios. (a)10x；(b)50x；(c)100x；(d)500xFig.17 The reconstruction results of different filter holograms at different attenuation lengths (a)Butterworth low-pass filter;(b)Ideal low pass filter;(c)Gaussian low pass filterFig.18. Comparison of different filter reconstruction indexes of holograms at different attenuations.（a）SSIM;（b）PSNR（c）RMSEFig.19. Reconstruction results of maximum attenuation length.(a)10.4AL;(b)10.3AL</dc:description>
  <dc:subject>digital holography; scattering imaging;  image processing</dc:subject>
  <dc:creator>Ying Jin</dc:creator>
  <dc:creator>Quan Liu</dc:creator>
  <dc:creator>Guohai Situ</dc:creator>
  <dc:creator>Quanying Wu</dc:creator>
  <dc:rights>RESTRICTED</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:publisher>Science Data Bank</dc:publisher>
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