Signal to noise ratio based filter optimization in triple energy window scatter correction

Triple energy window (TEW) scatter correction estimates the contribution of scattered photons to the acquisition data by acquiring additional data through two narrow energy windows placed adjoined to the main (photopeak) energy window. The contribution is estimated by linear interpolation and then s...

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Veröffentlicht in:Medical physics (Lancaster) 2000-08, Vol.27 (8), p.1955-1960
Hauptverfasser: Blokland, Koos (J.) A. K., Winn, R. D. R., Pauwels, E. K. J.
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container_end_page 1960
container_issue 8
container_start_page 1955
container_title Medical physics (Lancaster)
container_volume 27
creator Blokland, Koos (J.) A. K.
Winn, R. D. R.
Pauwels, E. K. J.
description Triple energy window (TEW) scatter correction estimates the contribution of scattered photons to the acquisition data by acquiring additional data through two narrow energy windows placed adjoined to the main (photopeak) energy window. The contribution is estimated by linear interpolation and then subtracted. Noise amplification is reduced by filtering both the photopeak scintigram and the scatter estimate. We have studied the filter settings of each filter using a physical phantom filled with a 201 Tl -solution resulting in count densities comparable to clinical studies. The performance of order-8 Butterworth filters at different cut-off frequencies (CoFs) were compared based on signal to noise ratios (SNRs). The highest SNRs were obtained when the noisy scatter information was strongly filtered with the CoF less than or equal to 0.07 cycles/pixel (cpp). The best CoF for the filter of the photopeak image is object size dependent; smaller objects require a higher CoF. For objects with a size near the SPECT spatial resolution (∼15 mm) the optimal CoF is equal to 0.18 cpp. For larger objects (31.8 mm) the highest SNR was obtained with a CoF equal to 0.13 cpp. A CoF equal to 0.16 cpp is a good compromise for all objects with a diameter equal to the spatial resolution or larger. These results depend on the initial signal to noise ratio of the acquisition data and so on the count density.
doi_str_mv 10.1118/1.1287286
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J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Signal to noise ratio based filter optimization in triple energy window scatter correction</atitle><jtitle>Medical physics (Lancaster)</jtitle><addtitle>Med Phys</addtitle><date>2000-08</date><risdate>2000</risdate><volume>27</volume><issue>8</issue><spage>1955</spage><epage>1960</epage><pages>1955-1960</pages><issn>0094-2405</issn><eissn>2473-4209</eissn><coden>MPHYA6</coden><abstract>Triple energy window (TEW) scatter correction estimates the contribution of scattered photons to the acquisition data by acquiring additional data through two narrow energy windows placed adjoined to the main (photopeak) energy window. The contribution is estimated by linear interpolation and then subtracted. Noise amplification is reduced by filtering both the photopeak scintigram and the scatter estimate. 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source MEDLINE; Access via Wiley Online Library
subjects Butterworth filters
filters
Image Processing, Computer-Assisted - methods
interpolation
Interpolation
curve fitting
Medical imaging
Models, Statistical
Noise
noise reduction
Phantoms, Imaging
Photon scattering
Photons
Physicists
random noise
scatter correction
Scattering, Radiation
single photon emission computed tomography
Single photon emission computed tomography (SPECT)
Spatial resolution
SPECT
Tomography, Emission-Computed, Single-Photon - methods
triple energy window
title Signal to noise ratio based filter optimization in triple energy window scatter correction
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