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Enhanced cross‐talk correction technique for simultaneous dual‐isotope imaging: A TL‐201/Tc‐99m myocardial perfusion SPECT dog study
Author(s) -
Knešaurek Karin,
Machac Josef
Publication year - 1997
Publication title -
medical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.473
H-Index - 180
eISSN - 2473-4209
pISSN - 0094-2405
DOI - 10.1118/1.598105
Subject(s) - isotope , physics , thallium , imaging phantom , nuclear medicine , contrast (vision) , spect imaging , optics , materials science , nuclear physics , medicine , metallurgy
A newly developed cross‐talk correction method for simultaneous dual‐isotope SPECT imaging was tested in a canine model. The method is based on the assumption that the transformations, which modify the primary energy window images into the scatter images as viewed in the other energy windows, are known. These transformations were found by measuring the point spread functions (PSFs) in two different energy windows for both isotopes in water. The dual‐isotope correction method is described by two convolution equations which were applied in frequency space. The equations take into account the different spatial distributions of the primary and scatter cross‐talk photons. The new enhancement of the method was in applying restoration filters to the resulting corrected images. Three separate studies were acquired in our dog study: two single‐isotope and one dual‐isotope study. The single isotope images were used as references. The contrast between the left ventricle cavity (LVC) and the myocardium was used in transaxial and short‐axis slices as a parameter to evaluate results of dual‐isotope correction method with restoration. The change in contrast in the dual‐isotope corrected images in both energy windows, i.e., Tc‐99m primary window (140 keV) and Tl‐201 primary window (70 keV), was significant. The only exception was for the short‐axis Tc‐99m window images. The corrected 140 keV dual‐isotope short‐axis slice had the contrast of 0.60 vs 0.58, which was the value in the noncorrected dual‐isotope short‐axis slice. For dual‐isotope 140 keV transaxial slice, the contrast changed from 0.72 to 0.82 after correction. In comparison, for single‐isotope Tc‐99m 140 keV transaxial slice, contrast changed from 0.62 to 0.84 after restoration correction. There was less change in contrast in the short‐axis Tc‐99m 140 keV slice, i.e., from 0.56 to 0.61. In the Tl‐201 primary window for the transaxial slices the improvement of contrast was from 0.38 to 0.64, and for short‐axis slices from 0.22 to 0.32 after correction. In the same 70 keV energy window for single‐isotope Tl‐201 images, contrast improved from 0.61 to 0.69 and from 0.35 to 0.38 for transaxial and short‐axis slice, respectively, after applying restoration correction. In conclusion, the presented dual‐isotope correction method with restoration improves the quality of the simultaneous rest Tl‐201/stress Tc‐99m sestamibi SPECT imaging.