Investigation of Scatter and Septal Penetration in I-131 Imaging Using GATE Simulation.
- Author:
Ji Young JUNG
1
;
Hee Joung KIM
;
A Ram YU
;
Hyo Min CHO
;
Chang Lae LEE
;
Hye Suk PARK
Author Information
1. Department of Radiological Science, College of Health Science and Research Institute of Health Science, Yonsei University, Wonju, Korea. hjk1@yonsei.ac.kr
- Publication Type:Original Article
- Keywords:
I-131;
GATE;
Septal penetration;
TEW;
ETEW
- MeSH:
Gamma Cameras;
Rejection (Psychology);
Water
- From:Korean Journal of Medical Physics
2009;20(2):72-79
- CountryRepublic of Korea
- Language:Korean
-
Abstract:
Scatter correction for I-131 plays a very important role to improve image quality and quantitation. I-131 has multiple and higher energy gamma-ray emissions. Image quality and quantitative accuracy in I-131 imaging are degraded by object scatter as well as scatter and septal penetration in the collimator. The purpose of this study was to estimate scatter and septal penetration and investigate two scatter correction methods using Monte Carlo simulation. The gamma camera system simulated in this study was a FORTE system (Phillips, Nederland) with high energy, general-purpose, parallel hole collimator. We simulated for two types of high energy collimators. One is composed of lead, and the other is composed of artificially high Z number and high density. We simulated energy spectrum using a point source in air. We estimated both full width at half maximum (FWHM) and full width at tenth maximum (FWTM) using line spread function (LSF) in cylindrical water phantom. We applied two scatter correction methods, triple energy window scatter correction (TEW) and extended triple energy window scatter correction (ETEW). The TEW method is a pixel-by pixel based correction which is easy to implement clinically. The ETEW is a modification of the TEW which corrects for scatter by using abutted scatter rejection window, which can overestimate or the underestimate scatter. The both FWHM and FWTM were estimated as 41.2 mm and 206.5 mm for lead collimator, respectively. The FWHM and FWTM were estimated as 27.3 mm and 45.6 mm for artificially high Z and high density collimator, respectively. ETEW showed that the estimation of scatter components was close to the true scatter components. In conclusion, correction for septal penetration and scatter is important to improve image quality and quantitative accuracy in I-131 imaging. The ETEW method in scatter correction appeared to be useful in I-131 imaging.
