Performance evaluation of a large axial field-of-view PET scanner: SET-2400W

The SET-2400W is a newly designed whole-body PET scanner with a large axial field of view (20 cm). Its physical performance was investigated and evaluated. The scanner consists of four rings of 112 BGO detector units (22.8 mm in-plane × 50 mm axial × 30 mm depth). Each detector unit has a 6 (in-plane) × 8 (axial) matrix of BGO crystals coupled to two dual photomultiplier tubes. They are arranged in 32 rings giving 63 two-dimensional image planes. Sensitivity for a 20-cm cylindrical phantom was 6.1 kcps/kBq/m/ (224 kcps/μCi/ml) in the 2D clinical mode, and to 48.6 kcps/kBq/ ml (1.8 Mcps/μCi/ml) in the 3D mode after scatter correction. In-plane spatial resolution was 3.9 mm FWHM at the center of the field-of-view, and 4.4 mm FWHM tangentially, and 5.4 mm FWHM radially at 100 mm from the center. Average axial resolution was 4.5 mm FWHM at the center and 5.8 mm FWHM at a radial position 100 mm from the center. Average scatter fraction was 8% for the 2D mode and 40% for the 3D mode. The maximum count rate was 230 kcps in the 2D mode and 350 kcps in the 3D mode. Clinical images demonstrate the utility of an enlarged axial field-of-view scanner in brain study and whole-body PET imaging.

[1]  J. Colsher,et al.  Fully-three-dimensional positron emission tomography , 1980, Physics in medicine and biology.

[2]  M. Mintun,et al.  Development Of Scatter Correction Techniques For Quantitative 3D Rviaging In A Whole Body PET Scanner With The Septa Retracted , 1993, 1993 IEEE Conference Record Nuclear Science Symposium and Medical Imaging Conference.

[3]  G Muehllehner,et al.  Singles transmission in volume-imaging PET with a 137Cs source. , 1995, Physics in medicine and biology.

[4]  E. Hoffman,et al.  Performance standards in positron emission tomography. , 1991, Journal of nuclear medicine : official publication, Society of Nuclear Medicine.

[5]  A Geissbuhler,et al.  Implementation of three-dimensional image reconstruction for multi-ring positron tomographs. , 1990, Physics in medicine and biology.

[6]  T. Spinks,et al.  Correction for scatter in 3D brain PET using a dual energy window method. , 1996, Physics in medicine and biology.

[7]  T G Turkington,et al.  Performance characteristics of a whole-body PET scanner. , 1994, Journal of nuclear medicine : official publication, Society of Nuclear Medicine.

[8]  E. Hoffman,et al.  Fully three-dimensional reconstruction for a PET camera with retractable septa , 1991 .

[9]  S R Meikle,et al.  A convolution-subtraction scatter correction method for 3D PET. , 1994, Physics in medicine and biology.

[10]  Iwao Kanno,et al.  A New PET Camera for Noninvasive Quantitation of Physiological Functional Parametric Images , 1996 .

[11]  S R Cherry,et al.  Attenuation correction using count-limited transmission data in positron emission tomography. , 1993, Journal of nuclear medicine : official publication, Society of Nuclear Medicine.

[12]  I Kanno,et al.  Deadtime correction method using random coincidence for PET. , 1986, Journal of nuclear medicine : official publication, Society of Nuclear Medicine.

[13]  S R Cherry,et al.  3D PET using a conventional multislice tomograph without septa. , 1991, Journal of computer assisted tomography.

[14]  S Grootoonk,et al.  Performance Evaluation of the Positron Scanner ECAT EXACT , 1992, Journal of computer assisted tomography.

[15]  Iwao Kanno,et al.  Design and evaluation of HEADTOME-IV, a whole-body positron emission tomograph , 1989 .

[16]  K Wienhard,et al.  The ECAT EXACT HR: Performance of a New High Resolution Positron Scanner , 1994, Journal of computer assisted tomography.