Characterization of dual layer phoswich detector performance for small animal PET using Monte Carlo simulation.

A positron emission tomograph dedicated to small animal imaging should have high spatial resolution and sensitivity, and dual layer scintillators have been developed for this purpose. In this study, simulations were performed to optimize the order and the length of each crystal of a dual layer phoswich detector, and to evaluate the possibility of measuring signals from each layer of the phoswich detector. A simulation tool GATE was used to estimate the sensitivity and resolution of a small PET scanner. The proposed scanner is based on dual layer phoswich detector modules arranged in a ring of 10 cm diameter. Each module is composed of 8 x 8 arrays of phoswich detectors consisting of LSO and LuYAP with a 2 mm x 2 mm sensitive area coupled to a Hamamatsu R7600-00-M64 PSPMT. The length of the front layer of the phoswich detector varied from 0 to 10 mm at 1 mm intervals, and the total length (LSO + LuYAP) was fixed at 20 mm. The order of the crystal layers of the phoswich detector was also changed. Radial resolutions were kept below 3.4 mm and 3.7 mm over 8 cm FOV, and sensitivities were 7.4% and 8.0% for LSO 5 mm-LuYAP 15 mm, and LuYAP 6 mm-LSO 14 mm phoswich detectors, respectively. Whereas, high and uniform resolutions were achieved by using the LSO front layer, higher sensitivities were obtained by changing the crystal order. The feasibilities for applying crystal identification methods to phoswich detectors consisting of LSO and LuYAP were investigated using simulation and experimentally derived measurements of the light outputs from each layer of the phoswich detector. In this study, the optimal order and lengths of the dual layer phoswich detector were derived in order to achieve high sensitivity and high and uniform radial resolution.

[1]  Simon R. Cherry,et al.  Design studies of a high resolution PET detector using APD arrays , 2000 .

[2]  J. G. Rogers,et al.  Segmented LSO crystals for depth-of-interaction encoding in PET , 1997 .

[3]  Magnus Dahlbom,et al.  Performance of a YSO/LSO phoswich detector for use in a PET/SPECT system , 1997 .

[4]  P. Bartzakos,et al.  A depth-encoded PET detector , 1990 .

[5]  S. Cherry,et al.  Performance evaluation of microPET: a high-resolution lutetium oxyorthosilicate PET scanner for animal imaging. , 1999, Journal of nuclear medicine : official publication, Society of Nuclear Medicine.

[6]  H. Murayama,et al.  Depth encoding multicrystal detectors for PET , 1998 .

[7]  Horst Halling,et al.  Pulse shape discrimination of LSO and LuYAP scintillators for depth of interaction detection in PET , 2002 .

[8]  Jurgen Seidel,et al.  Resolution uniformity and sensitivity of the NIH ATLAS small animal PET scanner: comparison to simulated LSO scanners without depth-of-interaction capability , 2001 .

[9]  C. Comtat,et al.  Monte Carlo Simulation for the ECAT EXACT HR+ system using GATE , 2003, IEEE Transactions on Nuclear Science.

[10]  D. Wolski,et al.  Properties of the new LuAP:Ce scintillator , 1997 .

[11]  S S Gambhir,et al.  Use of positron emission tomography in animal research. , 2001, ILAR journal.

[12]  Michael V. Green,et al.  Depth identification accuracy of a three layer phoswich PET detector module , 1999 .

[13]  C. Melcher,et al.  Cerium-doped lutetium oxyorthosilicate: a fast, efficient new scintillator , 1991, Conference Record of the 1991 IEEE Nuclear Science Symposium and Medical Imaging Conference.

[14]  W. Moses,et al.  A room temperature LSO/PIN photodiode PET detector module that measures depth of interaction , 1995 .

[15]  Uwe Pietrzyk,et al.  Design optimization of the PMT-ClearPET prototypes based on simulation studies with GEANT3 , 2002 .

[16]  Paul Lecoq,et al.  New inorganic scintillation materials development for medical imaging , 2001 .

[17]  I Buvat,et al.  Validation of the GATE Monte Carlo simulation platform for modelling a CsI(Tl) scintillation camera dedicated to small-animal imaging , 2004, Physics in medicine and biology.

[18]  Ignace Lemahieu,et al.  Monte Carlo simulations of a scintillation camera using GATE: validation and application modelling. , 2003, Physics in medicine and biology.

[19]  Klaus Wienhard,et al.  The ECAT HRRT: performance and first clinical application of the new high resolution research tomograph , 2000 .

[20]  R S Balaban,et al.  Challenges in small animal noninvasive imaging. , 2001, ILAR journal.

[21]  G. Santin,et al.  GATE: a Geant4-based simulation platform for PET and SPECT integrating movement and time management , 2003 .