Development of a High Precision Axial 3-D PET for Brain Imaging

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Development of a High Precision Axial 3-D PET for Brain Imaging On behalf of the AX-PET Collaboration SIENA - IPRD08 October 1st 4th, 2008 1

Outline Basics of Positron Emission Tomography (PET); Principle of the AX-PET scanner; Recent progress towards a Two-Module Demonstrator: LYSO Crystals; Wave Length Shifter (WLS) Strips; Photo Detectors (MPPC); Axial coordinate Reconstruction; Outlook. 2

Positron Emission Tomography (PET) Images of functional processes in the body; Injection of biologically active molecules (FDG-FluoroDeoxyGlucose), tagged with radioactive (β+) tracers -> 18F, 11C, 15O ; β+ annihilation with e from tissue, forming back-to-back 511 kev photon pair; Detection of the photon pair (Line of Response) by means of a set of detectors surrounding the patient; Display of areas with high metabolic activity by means of intersections of Lines of Response; Reconstruct 2D/3D images. 3

Standard (radial) PET scanners Photon pair detection efficiency: Very important (related to the quantity of radioactive dose to inject to the patient); Depends on: - length of the crystals L; - attenuation length of the crystals λ a;l 2 λ ε 2 = 1 e a L Typical crystal attenuation length: 1-2 cm; λa εscanner Recent L = PET (HRRT, Knoxville, USA) efficiency 2 ~ 40%; L = detection 2 λa ε2 ~ 75%; for the of photon pairs is given to be 6.9%. K.Wienhard et al., IEEE TNS 49 (2002) 104-110 4

Standard (radial) PET scanners Depth of Interaction (DOI): Is not measured; Introduces a parallax error; δ p = L sin α L The resolution degrades with L; The resolution in the off-center region degrades significantly; HRRT PET volumetric resolution is given as 20 mm3 FWHM. Solution: δp α Measure DOI, changing the geometry Use of long crystals oriented parallel to the scanner axe; Use wave length shifting strips (WLS) to read the third coordinate. 5

Axial PET geometry 6

Crystal + WLS The Principle: Catch the scintillation light which is lost outside the angle of total reflection in the crystal to produce wave length shifted light in the WLS strip; X and Y coordinates (resolutions) are derived by the crystal (dimensions); Z coordinate (resolution) is derived by the (width of the) WLS strip; Read-out one end of WLS strips and crystals. Reflector on opposite side; Resolution in all three coordinates can be chosen, without compromising on the photon pair detection efficiency; Detection of Compton cascades is possible increase of the total efficiency up to 13.6%-15.3%, depending on the recoil electron energy 7 cut-off.

PET Detector Demonstrator Two PET Modules under construction 6 layers of 8 LYSO crystal bars per module; Interleaved with 26 WLS strips oriented perpendicular to the crystal axe; Read-out with MPPC; Evaluation of all aspects of the concept by mounting the 2 modules at 1800 on a turntable gantry with a suitable phantom. Photon pair detection efficiency adjustable by selecting the number of layers; 8

The LYSO crystals Produced by Saint-Gobain Crystals; Optical polishing an all sides; Dimension: 3x3x100 mm3; LYSO Specification: Density: 7.1 g/cm3; Light yield > 25 ph/kev; Hygroscopic: no; Refractive index: 1.81; Light decay time: 41 ns; Intrinsic energy resolution: 9 IPRD08, 1-4 October 2008, Siena, Italy 7-8% FWHM; Attenuation length for 511 kev: 1.2 cm;

Experimental set-up for LYSO characterization 1 PMT Photonis XP2978 + BaF2 LYSO Bar + 2 PMTs BURLE 8850 22 PMTs Pb collimator Na source linear M-511n(Phys.Instrum. ) coupled to+ the LYSO bar through opticaltranslator grease (BC-630, index = 1.47) 10

Typical LYSO measurements PMT LEFT PMT RIGHT 1050 1,1 1000 950 900 y = m1*exp(m0/m2) Value Error m1 877,3 2,792 m2 40,632 0,9445 Chisq 69,372 NA R 0,98171 NA 850 y = m1*exp(-m0/m2) Value Error m1 1109,2 3,313 m2 44,181 1,1184 Chisq 27,697 NA R 0,99123 NA 1,05 RATIO 1 y = m1*exp(-2*m0/m2) Value Error m1 1,2608 0,0054769 m2 42,814 0,73811 Chisq 18,618 NA R 0,99723 NA 0,95 0,9 0,85 800 0 1,15 RATIO To evaluate the effective light attenuation length (λeff) the 22Na source is positioned at 7 positions; ADC Channels 1,2 1100 2 4 6 Pos (cm) 8 10 0 2 4 6 Pos (cm) 8 96 samples measured: λeff at 511 kev: (41.4 ± 2.6) cm; Energy resolution E/E at 511 kev in the middle of the crystal: (11 ± 0.4)% FWHM; Npe at 511 kev in the middle of the crystal: 1165 ± 64; 11 10

WLS Strips (ELJEN EJ-280) The fluorescent light is shifted from blue into the green range with a peak emission at 490 nm; The density of the plastic material is 1.02 g/cm3; The quantum efficiency of the fluorescent dye is 0.86 and its decay time 8.5 ns; Dimension: 0.9x3x40 mm3; 12

WLS Measurements Measured transmission coefficient for three thicknesses (0.7 mm, 1.1 mm and 1.5 mm); Verified absorption of blue light and emission of the green one; Measured WLS light output with a PMT at the end of a strip; For 61 samples light output: (48 ± 2) Npe with a λeff: (160 ± 7) mm; On average a loss of 6 p.e. over 25 mm. 32.5mm 7 WLS 2 PMT 7.5mm 13

MPPC (Multi Pixel Photon Counter) Produced by Hamamatsu; High Gain (105 @ HV=-70V); High PDE; Immune to B-field (NMR); LYSO readout: 3 x 3 mm2 active area; 3600 pixels (size 50 x 50 µm2); Ceramic package; First 50 samples have been recently delivered; WLS readout: 1.19 x 3.22 mm2 active area; 782 pixels (70 x 70 μm2 pixel size); Plastic package; 500 pieces delivered in July. IPRD08, 1-4 October 2008, Siena, Italy 14

Samples of 3 x 3 mm2 MPPC (for LYSO read out) have been tested; Not yet available measurements on 1.19 x 3.22 mm2 MPPC (for WLS read out); Charge gain, dark count rate and optical cross-talk are plotted as function of the applied bias voltage; Relative detection efficiency to detect one ore more photoelectrons, obtained from the zero count rate, is plotted versus the bias voltage (plateau @ -71V). Relative Detection Efficiency MPPC Measurements 15

Reconstruction of Axial Coordinate GEANT4 software package is used and developed; Optimize simulation based on measured data using an electron beam; Axial resolution using center of gravity (strip with highest signal ± 2 neighbors): ~1 mm FWHM volumetric precision ~5 mm3 FWHM; 16

Outlook Proof of concept looks very encouraging; All key components (LYSO Crystals, WLS strips and MPPC) tested (promising results); The projected spatial resolution will result in a volumetric precision of ~5 mm3 FWHM, close to the limits imposed by the physics of the positron decay (non-colinearity and positron range); A two module demonstrator with altogether 408 channels is under development: Electronics is under development; Mechanics is in production; Demonstration of the feasibility of the project, reconstructing the image of the phantom brain, expected in 2009. 17

Thanks for your attention! 18

19

Compton enhanced reconstruction Interactions <170 kev has to be primary Interactions >170 kev can be Compton or photoabsorption 20

Small scale lab test setup MPPC, LYSO and WLS with AX-PET dimensions in same setup 2nd scintillator to tag 511keV from Na-22 Reading out 8 WLS MPPC Na-22 Scintillator PMT 21

Small scale lab test setup LYSO energy resolution: 12% FWHM WLS output: 73 p.e. @ 511keV in 1 WLS LYSO Good agreement with previous measurements and simulations! WLS 22