A hybrid scatter correction for 3D PET based on an estimation of the distribution of unscattered coincidences:: implementation on the ECAT EXACT HR

被引:22
作者
Ferreira, NC
Trébossen, R
Lartizien, C
Brulon, V
Merceron, P
Bendriem, B
机构
[1] Serv Hosp Frederic Joliot, F-91406 Orsay, France
[2] Univ Coimbra, Fac Med, Serv Biofis, P-3000 Coimbra, Portugal
[3] CTI PET Syst Inc, Knoxville, TN 37932 USA
关键词
D O I
10.1088/0031-9155/47/9/310
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
We implemented a hybrid scatter-correction method for 3D PET that combines two scatter-correction methods in a complementary way. The implemented scheme uses a method based on the discrimination of the energy of events (the estimation of trues method (ETM)) and an auxiliary method (the single scatter simulation method (SSS 1) or the convolution-subtraction method (CONV)) in an attempt to increase the accuracy of the correction over a wider range of acquisitions. The ETM takes into account the scatter from outside the field-of-view (FOV), which is not estimated with the auxiliary method. On the other hand, the auxiliary method accounts for events that have scattered with small angles, which have an energy that cannot be discriminated from that of unscattered events using the ETM. The ETM uses the data acquired in an upper energy window above the photopeak (550-650 keV) to obtain a noisy estimate of the unscattered events in the standard window (350-650 keV). Our implementation uses the auxiliary method to correct the residual scatter in the upper window. After appropriate scaling, the upper window data are subtracted from the total coincidences acquired in the standard window, resulting in the final scatter estimate, after smoothing. In this work we compare the hybrid method with the corrections used by default in the 2D and 3D modes of the ECAT EXACT HR+ using phantom measurements. Generally, the contrast was better with the hybrid method, although the relative errors of quantification were similar. We conclude that hybrid techniques such as the one implemented in this work can provide an accurate, general-purpose and practical way to correct the scatter in 3D PET, taking into account the scatter from outside the FOV.
引用
收藏
页码:1555 / 1571
页数:17
相关论文
共 23 条
[1]   Energy-based scatter correction for 3-D PET scanners using NaI(Tl) detectors [J].
Adam, LE ;
Karp, JS ;
Freifelder, R .
IEEE TRANSACTIONS ON MEDICAL IMAGING, 2000, 19 (05) :513-521
[2]   A CONVOLUTION-SUBTRACTION SCATTER CORRECTION METHOD FOR 3D PET [J].
BAILEY, DL ;
MEIKLE, SR .
PHYSICS IN MEDICINE AND BIOLOGY, 1994, 39 (03) :411-424
[3]  
BENDRIEM B, 1993, P IEEE MED IM C SAN, V3, P1779
[4]  
Brix G, 1997, J NUCL MED, V38, P1614
[5]  
Casey M. E., 1995, Proceedings of the 1995 International Meeting on Fully Three-Dimensional Image Reconstruction in Radiology and Nuclear Medicine, P67
[6]  
CASTIGLIONI I, 1999, P INT M FULL 3D IM R, P337
[7]  
DAUBEWITHERSPOO.ME, 1998, P IEEE NUCL SCI S ME, V2, P1237
[8]   Influence of malfunctioning block detectors on the calculation of single detector efficiencies in PET [J].
Ferreira, NC ;
Trébossen, R ;
Grégoire, MC ;
Bendriem, B .
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, 1999, 46 (04) :1062-1069
[9]   Iterative crystal efficiency calculation in fully 3-D PET [J].
Ferreira, NC ;
Trébossen, R ;
Comtat, C ;
Grégoire, MC ;
Bendriem, B .
IEEE TRANSACTIONS ON MEDICAL IMAGING, 2000, 19 (05) :485-492
[10]  
GOGGIN AS, 1994, P IEEE NUCL SCI S ME, V4, P1609