Outline PET Systems: Instrumentation and Data Acquisition • Basics of PET Scanner Design • Review of Current PET Instrumentation Frederic H. Fahey DSc Children’s Hospital Boston Harvard Medical School frederic.fahey@childrens.harvard.edu Positron Emission Detector Ring 18F + 511 keV e511 keV 1 Detector Blocks (GE Advance NXi) Large Crystal Designs •Large NaI detectors, PMT array •25x50 cm, 1” thick •Hexagonal array True, Scatter and Random Coincidence Detections New Detector Materials SCINTILLATOR Rel. Light Yield True Scatter NaI(Tl) 100 Peak Wavelength (nm) 410 BGO LSO GSO 15-20 75 20-25 480 420 440 Decay Constant (ns) 230 300 12,42 30-60 Density (g/cc) 3.67 7.13 7.40 6.71 51 75 66 59 Index of Refraction 1.85 2.15 1.82 1.85 Hygroscopic ? Yes No No No Effective Z Random (R = 2 τ N1 N2) 2 18 17 16 15 14 13 12 11 10 9 8 7 6 5 4 3 2 1 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 * * * * * * * 15 * * * * * * * 14 * * * * * * * 13 * * * * * * * 12 * * * * * * * 11 * * * * * * * 10 * * * * * * * 9 * * * * * * * 8 * * * * * * * 7 * * * * * * 6 * * * * * 5 4 3 2 1 * * * * 1 2 3 4 5 6 7 8 9 10 11 12 13 14 * * * * * * 15 * * * * * 16 * * * * 17 18 18 Span of 7 Michelogram 15 14 13 12 11 10 9 8 7 6 5 4 3 2 1 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 1 3D septa are removed * * * * * * * 16 16 2D * * * * * * * 17 Span of 3 Michelogram Acquisition Modes * * * * * * * 18 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 2 * * * * * * * * * * * * * * * * 3 * * * * * * * * * * * * * * * * 4 * * * * * * * * * * * * * * * * 5 * * * * * * * * * * * * * * * * 6 * * * * * * * * * * * * * * * * 7 * * * * * * * * * * * * * * * * 8 * * * * * * * * * * * * * * * * 9 * * * * * * * * * * * * * * * * 10 * * * * * * * * * * * * * * * * 11 * * * * * * * * * * * * * * * * 12 * * * * * * * * * * * * * * * * 13 * * * * * * * * * * * * * * * * 14 * * * * * * * * * * * * * * * * 15 Segment 2 16 Segment 1 Segment 3 3 PET Attenuation Correction 3D PET P2 = e-µ(L-x) • • • • • Sensitivity drops off towards edges 4-5X increased sensitivity overall Increased scatter (15% to 40%) Increased randoms from out-of-field activity Rebinning algorithms to apply 2D reconstruction • Some devices can acquire in 2D or 3D whereas some can only acquire in 3D • 3D in Brain, 2D (or 3D) in Whole Body X P1 = e-µx PET Attenuation Correction Methods • Calculated – No noise but possibly inaccurate • Measured – Accurate but noisy • Segmented, Measured – Less noise => less time • Singles • CT L PTOT = P1 x P2 = e-µL Measured Attenuation Correction 100 20 Blank C Transmission Emission Corrected Emission = (Blank/Transmission) * Emission = (100/20) * C 4 Segmented, Measured Attenuation Correction •Noise added from measured attenuation correction •Rel err in unif phantom (10 min EM) •9% with calc atten •16% with 10 min TR •18% with 5 min TR •Segmentation classifies by tissue type •Smoothes lung areas •Substantial reduction in noise added Measured Singles-Based Attenuation Correction •Single-photon source (Cs-137) •Source shielded from “near”detectors •Energy resolution (NaI) allows separation of 2 peaks •High count rate reduces noise •Susceptible to scatter Segmented PET-CT Attenuation Correction PET-CT Attenuation Correction 5 PET Instrumentation • • • • High-Resolution Medium-Resolution PET-CT Special Purpose GE Advance NXi PET Instrumentation • High-Resolution – Siemens HR+ – GE Advance – Philips Allegro • Medium-Resolution – Siemens ACCEL – Philips CPET+ PET Instrumentation Detector Dimension (mm) # of Detectors Detector Material Spatial Resolution (mm) Sensitiv ity (kcps/uCi/mL) Siemens HR+ 4.1 x 4.4 x 30 18,432 BGO 4.6 200/900 GE Advance Philips Allegro 3.9 x 8.2 x 30 4 x 6 x 20 12,096 17,864 BGO GSO 4.8 4.8 200/1060 /800 Detector Dimension (mm) # of Detectors Detector Material Spatial Resolution (mm) Sensitivity (kcps/uCi/mL) Siemens Accel 6.8 x 6.8 x 20 9,216 LSO 6.2 180/780 Philips CPET+ 500x300x25 6 NaI 5 /450 6 GE Discovery ST PET-CT Scanners • • • • Siemens Biograph GE Discovery ST GE Discovery STE Philips Gemini CT PET-CT Scanners Detector Dimension (mm) # of PET Detectors PET Detector Material Spatial Resolution 2D/3D Atten Corr Detector Dimension (mm) # of PET Detectors PET Detector Material Spatial Resolution 2D/3D Atten Corr GE Discovery STE 4.7 x 6.3 x 30 13,440 BGO 5.0 2D/3D CT GE Discovery ST 6.2 x 6.2 x 30 10,080 BGO 6.1 2D/3D CT Siemens Biograph LSO Siemens Hi-Rez LSO 6.5 x 6.5 x 25 4 x 4 x 20 9,216 23,336 LSO LSO 6.3 4.6 3D 3D CT CT PET Special PET Devices Philips Gemini 4 x 6 x 20 17,864 GSO 4.9 3D CT&Cs-137 • Brain • Breast • Small Animal 7 Positron Emission Mammography (PEM) CTI ECAT HRRT • Max Planck Institute in Cologne • Dual LSO Phoswich for DOI Determination • Octagonal Design • 936 blocks with 128 2.1x2.1 dual detectors each • 120,000 crystals • Reconstructed resolution of less than 2.5 mm Courtesy of CTI Concorde MicroPET Scanner 650g Rat [18F] Fluoride 4 bed positions 30 min each Courtesy of Wake Forest University and PEM Technologies Summary • Scanners specifically optimized for clinical (oncologic) imaging • Sensitivity and count rate capability • New detector materials (faster!) • PET-CT • Special devices including small animal imaging Courtesy of Concorde MicroSystems 8