Thermoluminescent Properties of Cerium-Doped Lu2SO5 and Y2SiO5 Single Crystalline Films Scintillators Grown from PbO-B2O3 and Bi2O3 Fluxes

Kilian, A.; Bilski, P.; Gorbenko, V.; Zorenko, T.; Witkiewicz, Sandra; Paprocki, K.; Zorenko, Yuriy

doi:10.3390/cryst8030120

Cited by 6 publications

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References 30 publications

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“…In order to examine the influence of the crystal material on the information content of the final PET image, the system was also simulated by replacing the BGO crystal arrays with crystals of various quantum detection efficiency (QDE) [45] values, i.e., yttrium orthoaluminate perovskite (YAlO 3 :Ce or YAP, QDE = 0.75) [36,43,44], lutetium orthoaluminate perovskite LuAlO 3 :Ce or LuAP:Ce, lutetium yttrium orthoaluminate perovskite ((LuY)AlO 3 :Ce or LuYAP:Ce, QDE = 0.90) with 70% lutetium (Lu) atomic fraction, LuYAP:Ce with 80% Lu atomic fraction (QDE = 0.91) [44,46], lutetium oxyorthosilicate (Lu 2 SiO 5 :Ce or LSO, QDE = 0.93) [46][47][48][49][50], and gadolinium oxyorthosilicate (Gd 2 SiO 5 :Ce or GSO, QDE = 0.88) [43,44,51] crystals with dimensions equal to those of BGO (QDE = 0.94) (6.3 × 6.3 × 30 mm) in the tangential, axial, and radial directions, respectively.…”

Section: Modeled Pet System Geometrymentioning

confidence: 99%

Information Capacity of Positron Emission Tomography Scanners

et al. 2018

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Background: The aim of the present study was to assess the upper information content bound of positron emission tomography (PET) images, by means of the information capacity (IC). Methods: The Geant4 Application for the Tomographic Emission (GATE) Monte Carlo (MC) package was used, and reconstructed images were obtained by using the software for tomographic image reconstruction (STIR). The case study for the assessment of the information content was the General Electric (GE) Discovery-ST PET scanner. A thin-film plane source aluminum (Al) foil, coated with a thin layer of silica and with a 18F-fludeoxyglucose (FDG) bath distribution of 1 MBq was used. The influence of the (a) maximum likelihood estimation-ordered subsets-maximum a posteriori probability-one step late (MLE-OS-MAP-OSL) algorithm, using various subsets (1 to 21) and iterations (1 to 20) and (b) different scintillating crystals on PET scanner’s performance, was examined. The study was focused on the noise equivalent quanta (NEQ) and on the single index IC. Images of configurations by using different crystals were obtained after the commonly used 2-dimensional filtered back projection (FBP2D), 3-dimensional filtered back projection re-projection (FPB3DRP) and the (MLE)-OS-MAP-OSL algorithms. Results: Results shown that the images obtained with one subset and various iterations provided maximum NEQ values, however with a steep drop-off after 0.045 cycles/mm. The single index IC data were maximized for the range of 8–20 iterations and three subsets. The PET scanner configuration incorporating lutetium orthoaluminate perovskite (LuAP) crystals provided the highest NEQ values in 2D FBP for spatial frequencies higher than 0.028 cycles/mm. Bismuth germanium oxide (BGO) shows clear dominance against all other examined crystals across the spatial frequency range, in both 3D FBP and OS-MAP-OSL. The particular PET scanner provided optimum IC values using FBP3DRP and BGO crystals (2.4829 bits/mm2). Conclusions: The upper bound of the image information content of PET scanners can be fully characterized and further improved by investigating the imaging chain components through MC methods.

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