2017
DOI: 10.1109/tmi.2016.2606338
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Modeling and Pre-Treatment of Photon-Starved CT Data for Iterative Reconstruction

Abstract: An increasing number of X-ray CT procedures are being conducted with drastically reduced dosage, due at least in part to advances in statistical reconstruction methods that can deal more effectively with noise than can traditional techniques. As data become photon-limited, more detailed models are necessary to deal with count rates that drop to the levels of system electronic noise. We present two options for sinogram pre-treatment that can improve the performance of photon-starved measurements, with the inten… Show more

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Cited by 27 publications
(18 citation statements)
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“…We clipped nonpositive measurements by a threshold δ = 0.01 to enforce the logarithmic transform, which is the same as that in Wang et al . More advanced correction methods for nonpositive values may be favorable, but is out of the scope of this work. The corresponding images reconstructed by FBP and SIR‐ndiNLM [using Fig.…”
Section: Experiments and Resultsmentioning
confidence: 99%
“…We clipped nonpositive measurements by a threshold δ = 0.01 to enforce the logarithmic transform, which is the same as that in Wang et al . More advanced correction methods for nonpositive values may be favorable, but is out of the scope of this work. The corresponding images reconstructed by FBP and SIR‐ndiNLM [using Fig.…”
Section: Experiments and Resultsmentioning
confidence: 99%
“…Assuming both noise sources are independent and additive, we have a ‘Poisson+ Gaussian’ model [66] yi~Poissonfalse{αŷifalse}/α+Normalfalse{0,σ2false}, where y i and ŷ i are both in units of current-integrating DAS output, α is a scaling factor that converts the DAS output values to equivalent numbers of x-ray photons depending on the effective x-ray energy and the DAS gain, and σ 2 is the variance of the DAS electronic noise. σ 2 in modern CT DAS is typically equivalent to the counting statistics corresponding to from a handful [77][17][17][67][78] to a few hundred x-ray photons [65][37][13]. The parameters α and σ 2 can be measured by standard detector calibration processes [6].…”
Section: Statistical Modelsmentioning
confidence: 99%
“…In practice, smoothed or de-noised data can be used instead [38][31][36][32]. As an example, we implement a locally adaptive linear minimum mean squared-error (LLMMSE) filter very similar to what proposed by Chang, Zhang, Thibault, et al [78], where denoised data ӯ i , p̄ i and W̄ i , are used instead of the noisy data y i , p i , and W i . ӯi=maxfalse(denoisefalse(yifalse),δfalse). p¯i=fi1true(logIiӯitrue). W¯i=fifalse(p¯ifalse)2ӯi2ӯi+σα2. The smoothing radius of the LLMMSE filter is typically 3×3 or 6× 6 on a 2D detector.…”
Section: Statistical Modelsmentioning
confidence: 99%
“…First, the logarithm transform may lead the projection measurements become zero or negative due to electronic noise 53 . Several methods 54–56 were analyzed for dealing with nonpositive values. Second, estimating proper weight parameters in WLS methods is a challenging task.…”
Section: Introductionmentioning
confidence: 99%