Speaker
Prof.
Dimitris Maintas
(Institute of Isotopic Studies, Athens)
Description
The use of external positron emitting sources or single photon emitting sources at
energies similar to annihilation photons seems to give acceptable results
permitting the quantification of PET data. The attenuation correction based on CT
data generates artefacts around metallic prostheses, after use of contrast media
and in the pulmonary region near calcifications and on dense lesions. In the
present phantom study we investigated the density influence of simulated lesions on
attenuation correction based on CT transmission data. A cylindrical phantom of 21
cm diameter and 20 cm height, with two compartments, was used. The lower one with
cylinders of 4.0 to 10.0 mm to evaluate the resolution of the system and the upper
one with 3 pairs of cylindrical vials of 2.6cm diameter and 4.5 cm height,
positioned in a distance of 7 cm from the axis of the cylinder in a way to form an
hexagon. The first pair of vials was completed with alcohol solution (d= 0.8 g),
the second one with water (d= 1.0 g) and the third one with a KJ solution (d=
1.2g). The phantom’s lower part was filled with water and the upper with water or
polystyrene spheres plus water containing 18-FDG. In one vial of each pair equal
activities of 18-FDG were added, giving a ratio of 3 with the environment water or
water plus polystyrene. An initial acquisition by spiral CT was followed by one bed
acquisition of emission and external source transmission data. After reconstruction
by using filtered back projection for CT, iterative OSEM algorithms for PET and
scaling and segmentation attenuation correction procedures, proposed by the
constructors, we measured on transversal slices the activities of the 6 vials by
drawing similar ROIs over the vials and one ROI in the centre of the slices to
estimate the background activity. On non attenuation corrected (NAC) and CT
attenuation corrected (CTAC) images the measured and corrected for attenuation
activities are:
First tomograph NAC d=0.8: 571 counts d= 1.0 : 480 counts d=1.2: 430 counts
CTAC 4966 " 4853 " 7589 "
Second " NAC d=0.8: 850 counts d=1.0 : 661 counts d=1.2: 574 counts
CTAC 7421 " 7167 " 18343 "
Third NAC d=0.8: 700 counts d=1.0 : 620 counts d=1.2: 590 counts
CTAC 4900 " 3900 " 3300 "
In conclusion the activities on NAC images for all the 3 tomographs are inversely
depended on the density of the liquids due to more intense absorption by the denser
material. On CT attenuation corrected slices, in the two first tomographs, the
estimated activity in denser material of specific activity 1.2g is much higher than
the expected due to incorrect attenuation correction procedure. In the third
tomograph the CTAC has not the same correctional effect.
Author
Prof.
Dimitris Maintas
(Institute of Isotopic Studies, Athens)
Co-authors
Dr
Catherine Maintas
(CMN Pneumonological & Cardiological Hospital, Lyon)
Dr
Claire Houzard
(CMN Pmeumonological & Cardiological Hospital, Lyon)
Prof.
Daniel Slosman
(Institut of Nuclear Madicine, Clinique Generale BAULIEU, Geneva)
Dr
Florent Cachin
(Nuclear Medicine Department Centre Jean Perin, Clermont - Ferrand)
Dr
Gerard Galy
(CMN Pneumonological &Cardiological Hospital of Lyon)
Prof.
Roland Itti
(CMN, Pneumonological & Cardiological Hospital, Lyon)
Dr
Thomas Mogneti
(Nuclear Medicine Department Centr Leon Berard Lyon)