{"title":"Massively Parallel Spatially-Variant Maximum Likelihood Image Restoration","authors":"A. Boden, D. Redding, R. Hanisch, J. Mo","doi":"10.1364/srs.1995.rwb3","DOIUrl":null,"url":null,"abstract":"We consider a massively parallel implementation of Richardson-Lucy or maximum likelihood restoration with a spatially-variant point spread function (PSF). Richardson-Lucy iterates involve the computation of sums of the form: where O(x'\n q\n ) is the incident optical field estimate at discrete source location x'\n q\n , I(x\n q\n ) is the measured discrete image at discrete field location x\n q\n , and P(x\n q\n , x'\n q\n ) is the discrete PSF – the probability that a photon from source region x'\n q\n is incident on the detector at field region x\n q\n . In general P is a function of source and field coordinates, and the computational burden of Eq. 1 is intractably large.","PeriodicalId":184407,"journal":{"name":"Signal Recovery and Synthesis","volume":"106 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Signal Recovery and Synthesis","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/srs.1995.rwb3","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 6
Abstract
We consider a massively parallel implementation of Richardson-Lucy or maximum likelihood restoration with a spatially-variant point spread function (PSF). Richardson-Lucy iterates involve the computation of sums of the form: where O(x'
q
) is the incident optical field estimate at discrete source location x'
q
, I(x
q
) is the measured discrete image at discrete field location x
q
, and P(x
q
, x'
q
) is the discrete PSF – the probability that a photon from source region x'
q
is incident on the detector at field region x
q
. In general P is a function of source and field coordinates, and the computational burden of Eq. 1 is intractably large.