o D PET Scanner Quality Assurance Introduction Quality Control uc se od r ea p ou Pl e y R k ot n N a Th Procedures required to ensure that the distribution of radiation emitted from a patient is accurately reflected in the measured raw raw data. Brad Kemp, PhD Department of Radiology Mayo Clinic Facets • Quality assurance: – verify scanner is operating properly – identify problems prior to scanning patients • Acquisition of corrections to compensate for known imperfections in data measurement WE-A-330D-1 Outline • Corrections • System Calibration • Daily QA • NEMA NU 22-2001 Performance Standards System Correction: Normalization Purpose: Corrects for the variations in efficiency in lines of response (LOR) in each slice of the sinogram • A uniformity correction • For 2D: Direct Measurement using a low activity source • For 3D: Indirect Measurement using a uniform phantom • Acquired quarterly or after system maintenance • Scanner certification e 1 o D System Calibration Quality Assurance Quality Assurance Test Requirements • A phantom of known activity concentration is imaged and reconstructed with uniform attenuation correction • Average counts in a slice are calculated • Well defined regimen of measurements uc se od r ea p ou Pl e y R k ot n N a Th Purpose: convert image counts/pixel to activity/volume →From this a system calibration is calculated – Quick and easy to conduct – Sensitive to modes of failure of the scanner – Preferably quantitative, not qualitative • Acquired monthly or after system maintenance Blank Scan Quantitative Analysis of Blank Scans • On standstand-alone PET systems, used with transmission sinograms to create attenuation correction factors • Acquired daily - good source of QA data • Emission scan of uniform cylinder Transmission Sinograms Good blank Bad block Sinogram of a Uniform Cylinder • The quantitative analysis of blank scans is an important aspect of the QA of a PET scanner • Quantitative analysis of blank scans: - validates system calibration - provides information on crystal, block or module (bucket) efficiencies with respect to system average - compare to baseline - monitors system stability - ensures validity of normalization e 2 o D Quantitative Analysis of Blank Scans Overview: Daily QA Daily QA analysis calculates a global and slice normalized mean square error (NMSE) by using a reference scan; the reference scan is defined as the blank scan acquired immediately after normalization Time Line uc se od r ea p ou Pl e y R k ot n N a Th Normalization Normalization Reference Blank Daily Blank Has the system drifted? Is the normalization valid? Normalized Mean Square Error Quality Assurance Pixel to pixel comparison Reference Blank Daily Blank Detector and Electronics Characterization – Singles mode detector calibration • Crystal map • PMT gain adjustment • Energy map – Coincidence timing calibration ∑ (Counts − Counts ) NMSE = ∑ (Counts ) i i Did the engineer calibrate the scanner properly? DAY 2 i REF i REF 2 i Compute global and slice NMSE e 3 o D Verification of Crystal Map Crystal Map QA of crystal maps created during calibration of the scanner Purpose: • Map the position of the detected event to a specific crystal • Obtained quarterly or after detector maintenance uc se od r ea p ou Pl e y R k ot n N a Th Crystal Map Look Up Table Count distribution in a block PMT Gain Adjustment Coincidence Timing Calibration Purpose: Purpose: • Balances the gain characteristics of the PMTs in a block • Compensates for PMT gain drift with temperature, age, … • Acquired weekly (daily) or after detector maintenance • Adjust for timing delays so events from all blocks are timestamped equivalently • Acquired weekly (daily) or after detector maintenance 0.0 Update Gains Update Gains Block Bias (%) -1.0 -2.0 Morning -3.0 Afternoon -4.0 γ γ -5.0 Coincidence ? Yes Register Event -6.0 28-Feb 7-Mar 14-Mar 21-Mar 28-Mar Date e 4 o D Daily Quality Assurance Example: NMSE and Block Bias Can the Scanner be Used Today? QA must be sensitive to modes of failure of the scanner NMSE: Error with respect to baseline scan Potential Problems • System stability, drifts • Detector module / PMT/ preamp failure • Loose cables, connectors • Inoperable gantry motors, source loader 6 0.010 • Automatic PMT gain adjustment • Blank scan 4 2 0.006 0 -2 0.004 -4 0.002 -6 0.000 • QA will detect but not prevent these problems Block Bias (%) Normalized Mean Square Error uc se od r ea p ou Pl e y R k ot n N a Th Daily QA Regimen 0.008 Global NMSE Slice NMSE Block Bias 10-Dec-02 -8 29-Jan-03 20-Mar-03 9-May-03 28-Jun-03 17-Aug-03 Date Daily QA: Loose Cable Loose Cable Better QA Schedule Detector and Electronics Characterization – Crystal map – PMT gain – Coincidence timing Frequency Quarterly Weekly (daily) Weekly (daily) System Corrections Normalization – Scanner calibration – Blank Scan – Quarterly Monthly (weekly) Daily e 5 o D NEMA NU 2-2001 NEMA NU 2-2001 Acceptance Testing PET Performance Measurements Can we use our new scanner? uc se od r ea p ou Pl e y R k ot n N a Th National Electrical Manufacturers Association. NEMA Standards Publication NU 22-2001: Performance Measurements of Positron Emission Tomographs Annual QA Is the scanner still performing within specification? Phantoms for NU 2-2001 NEMA NU 22-2001 Performance Measures: Three phantoms: Scatter phantom 203x700mm phantom with activity in line source NEMA NU 2-2001 Sensitivity phantom • Spatial Resolution (Transaxial, axial) • Sensitivity • Scatter Fraction Image quality phantom • Count Losses • Count Rate Correction Accuracy • Image Quality e 6 o D Spatial Resolution Sensitivity • Spatial resolution of a system represents its ability to distinguish distinguish between two points of radioactivity uc se od r ea p ou Pl e y R k ot n N a Th • F-18 point sources in air at six locations: – (0,1), (0,10) and (10,0) cm – Center of axial FOV and ¼ axial FOV from center • Sensitivity of a scanner represents its ability to detect annihilation radiation • Rate of true coincidence counts per unit radioactivity (expressed (expressed in cps/kBq cps/kBq)) in absence of attenuating media • Rationale: need material around source to ensure annihilation of positrons, but this material also attenuates the annihilation photons • Based on technique by Bailey DL, Jones T, et al. Eur J Nucl Med 1991;18:3741991;18:374-379. • Reconstruct: image pixel < ⅓ expected FWHM • Profile width ~ 2 times FWHM • Report FWHM and FWTM in radial, tangential and axial directions Sensitivity Sensitivity • Successive measurements with a 700 mm line source with a known amount of FF-18 surrounded by nested, known absorbers • Measure at radial locations of 0 and 10cm • Report system sensitivity and slice sensitivity profile 2D 3D 0.05 Count Rate, R (cps) 1.5E+05 R0 1.0E+05 System Sensitivity = R0 Activity 0.03 0.02 R0 R10 0.01 0.00 0.30 R0 R10 0.20 0.10 0.00 0 5.0E+04 Sensitivity (cps/kBq) • The count rate with no absorber is extrapolated from these measures measures Sensitivity (cps/kBq) 0.40 0.04 10 20 30 Slice 40 50 0 10 20 30 40 50 Slice 0.0E+00 0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 Sleeve Thickness (cm) e 7 o D Scatter Fraction Scatter Fraction Scatter Fraction vs Slice • Scatter fraction is a measure of the system sensitivity to scatter scatter SF = Scatter Scatter + Trues 2D 20 3D 40 uc se od r ea p ou Pl e y R k ot n N a Th Scatter Fraction (%) Scatter Fraction (%) • Use 203 mm diameter polyethylene cylinder of length 700 mm, with activity located in a line source of diameter 2.3mm that is 4.5mm 4.5mm off axis • Measured with low activity (Randoms:Trues (Randoms:Trues = 1%) to avoid random coincidences, deadtime and pulse pileup. 35 15 10 5 30 25 20 15 10 5 0 0 0 10 20 30 40 50 0 10 Slice Count Rate Performance • Measurement of count rate performance gives an indication of scanner performance as a function of activity 30 40 50 Slice Count Rate Performance • Calculate Noise Equivalent Count Rate RNEC = • Use 700 mm long polyethylene cylinder • Measured with high initial activity of FF-18 3D: 800 MBq; MBq; 2D: 5 GBq • Acquire data until randoms and deadtime losses are negligible (14 to 18 hrs) 20 RTrues 2 RTrues + RScatter + k ⋅ RRandoms RNEC: Figure of merit relating scanner performance to sinogram SNR after randoms and scatter corrections. For NEMA, k = 1 (calculated Randoms); Randoms); RNEC (1R) • Report peak NEC and effective activity concentration at peak e 8 o D Count Rate Performance Image Quality Measurement Peak RTrues: 515 kcps @ 44 kBq/ml kBq/ml • Standardized imaging situation that simulates a clinical whole body imaging condition • Phantom consists of a torso phantom with hot and cold lesions in a warm background • Scatter phantom abutted to image quality phantom Peak RNEC (1R):118 kcps @ 22 kBq/ml kBq/ml Peak RNEC (2R): 80 kcps @ 18 kBq/ml kBq/ml NECR (1R) NECR (2R) 2500 2000 NECR (kcps) 120 3000 Count Rate (kcps) uc se od r ea p ou Pl e y R k ot n N a Th 140 3500 Prompts Trues R+S 1500 1000 500 100 80 60 40 20 0 0 0 10 20 30 40 50 60 Activity Concentration (kBq/cc) 0 10 20 30 Image Quality Measurement • • • • • • Hot spheres: 10, 13, 17, 22 mm id Cold spheres: 28, 37 mm id Lung insert Activity in hot spheres 8 and 4 times that of background Activity in background 5.3 kBq/ml kBq/ml Simulated acquisition 100cm in 60min Tacq = 40 50 60 Activity Concentration (kBq/cc) Image Quality Measurement • Report image contrast and SNRs for hot and cold lesions, residual error in lung, variability in background • Visual inspection for artifacts 60 min Δz ≈ 7 min 100 cm • Repeat acquisition three times • Reconstruct using clinical protocol e 9 o D NEMA and Lutetium-176 • LYSO is inherently radioactive • Background radiation gives rise to Randoms, Randoms, some Trues uc se od r ea p ou Pl e y R k ot n N a Th • Implications for NEMA: cannot obtain Randoms:Trues ratio of 1% • For count rate and sensitivity measurements – acquire delayed event to measure intrinsic randoms rates • Watson CC, et al. J Nucl Med 2004;45:8222004;45:822-826. • Erdi YE, et al. J Nucl Med 2004;45:8132004;45:813-821. e 10