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Impact of γ factor in the penalty function of Bayesian penalized likelihood reconstruction (Q.Clear) to achieve high-resolution PET images.

Authors :
Miwa, Kenta
Yoshii, Tokiya
Wagatsuma, Kei
Nezu, Shogo
Kamitaka, Yuto
Yamao, Tensho
Kobayashi, Rinya
Fukuda, Shohei
Yakushiji, Yu
Miyaji, Noriaki
Ishii, Kenji
Source :
EJNMMI Physics; 1/22/2023, Vol. 10 Issue 1, p1-12, 12p
Publication Year :
2023

Abstract

Background: The Bayesian penalized likelihood PET reconstruction (BPL) algorithm, Q.Clear (GE Healthcare), has recently been clinically applied to clinical image reconstruction. The BPL includes a relative difference penalty (RDP) as a penalty function. The β value that controls the behavior of RDP determines the global strength of noise suppression, whereas the γ factor in RDP controls the degree of edge preservation. The present study aimed to assess the effects of various γ factors in RDP on the ability to detect sub-centimeter lesions. Methods: All PET data were acquired for 10 min using a Discovery MI PET/CT system (GE Healthcare). We used a NEMA IEC body phantom containing spheres with inner diameters of 10, 13, 17, 22, 28 and 37 mm and 4.0, 5.0, 6.2, 7.9, 10 and 13 mm. The target-to-background ratio of the phantom was 4:1, and the background activity concentration was 5.3 kBq/mL. We also evaluated cold spheres containing only non-radioactive water with the same background activity concentration. All images were reconstructed using BPL + time of flight (TOF). The ranges of β values and γ factors in BPL were 50–600 and 2–20, respectively. We reconstructed PET images using the Duetto toolbox for MATLAB software. We calculated the % hot contrast recovery coefficient (CRC<subscript>hot</subscript>) of each hot sphere, the cold CRC (CRC<subscript>cold</subscript>) of each cold sphere, the background variability (BV) and residual lung error (LE). We measured the full width at half maximum (FWHM) of the micro hollow hot spheres ≤ 13 mm to assess spatial resolution on the reconstructed PET images. Results: The CRC<subscript>hot</subscript> and CRC<subscript>cold</subscript> for different β values and γ factors depended on the size of the small spheres. The CRC<subscript>hot,</subscript> CRC<subscript>cold</subscript> and BV increased along with the γ factor. A 6.2-mm hot sphere was obvious in BPL as lower β values and higher γ factors, whereas γ factors ≥ 10 resulted in images with increased background noise. The FWHM became smaller when the γ factor increased. Conclusion: High and low γ factors, respectively, preserved the edges of reconstructed PET images and promoted image smoothing. The BPL with a γ factor above the default value in Q.Clear (γ factor = 2) generated high-resolution PET images, although image noise slightly diverged. Optimizing the β value and the γ factor in BPL enabled the detection of lesions ≤ 6.2 mm. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
21977364
Volume :
10
Issue :
1
Database :
Complementary Index
Journal :
EJNMMI Physics
Publication Type :
Academic Journal
Accession number :
161417504
Full Text :
https://doi.org/10.1186/s40658-023-00527-w