2019
DOI: 10.3938/jkps.74.414
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Implementation of the Weighted L1-Norm Scatter Correction Scheme in Dual-Energy Radiography

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Cited by 3 publications
(3 citation statements)
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“…Such an approach could prove problematic in clinical practice since bony structures generate and absorb scatter differently from soft tissue. In 26 30 , the authors evaluated the image dehazing method proposed by Meng et al 31 to obtain a scatter map in radiography based on the alternating direction method of multipliers (ADMM) 32 . However, simultaneous correction of lungs and spine in chest radiography was not possible because of the need for a specific parameter that had to be empirically tuned depending on the intensity of each region.…”
Section: Introductionmentioning
confidence: 99%
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“…Such an approach could prove problematic in clinical practice since bony structures generate and absorb scatter differently from soft tissue. In 26 30 , the authors evaluated the image dehazing method proposed by Meng et al 31 to obtain a scatter map in radiography based on the alternating direction method of multipliers (ADMM) 32 . However, simultaneous correction of lungs and spine in chest radiography was not possible because of the need for a specific parameter that had to be empirically tuned depending on the intensity of each region.…”
Section: Introductionmentioning
confidence: 99%
“…However, simultaneous correction of lungs and spine in chest radiography was not possible because of the need for a specific parameter that had to be empirically tuned depending on the intensity of each region. Similar approaches were proposed for dual energy acquisitions, applying the ADMM algorithm prior to base material decomposition 30 .…”
Section: Introductionmentioning
confidence: 99%
“…Alternatively, decomposition methods use higher‐order models to associate the tissue maps corresponding to soft tissue and bone, x s and x b , with the natural logarithm of the measured photons at the detector over the total incident photons, d L and d H (second order, 9–13 third order 14–17 or other models such as conic and cubic surface equations 18 ):xs=false∑m=0Mn=0NqitalicmndLmdHn;xb=false∑m=0Mn=0NritalicmndLmdHndLts,tb=LnIL/NLεdε;dHts,tb=LnIH/NHεdεThe model parameters q mn and r mn can be obtained from a calibration step by acquiring different known combinations of x s and x b at low and high energies, which correspond to d L and d H . The equivalent materials used for the calibration need to resemble the attenuation of X‐rays by soft tissue and bone for different energies, which can be represented by the dual‐material dependency with the energy, DMD(x s , x b ) , shown in Fig.…”
Section: Introductionmentioning
confidence: 99%