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1
Physics & Instrumentation in
Positron Emission Tomography
Paul Vaska, Ph.D.
Center for Translational Neuroscience
Brookhaven National Laboratory
July 21, 2006
2
Non-invasive Medical Imaging
Techniques
Anatomical
• X-ray
• CAT
• MRI
• Ultrasound
Functional
• “nuclear medicine” - SPECT, PET
CAT
X-Ray
MRI
3
Positron Emission Tomography
Recent mainstream acceptance
- relatively expensive
- cyclotron for tracer production
- detectors must stop high-energy
gamma-rays
- low resolution (>2 mm), limited
counting statistics
- BUT unique functional capabilities
Applications
- Diagnosis of disease
- cancer (WB), cardiac, …
- Research
- brain function
- animal studies
4
Technical Challenges in PET Imaging
Radiochemistry - better tracers
Imaging Physics - better images by
• Detector design
– Spatial resolution
– Sensitivity
• Image processing
– Corrections for physical effects
– Image reconstruction algorithms
Data Analysis & Biological Modeling - better
interpretation of images
5
PET Imaging Overview
- Synthesize radiotracer
- Inject radiotracer
- Measure gamma-ray
emissions from isotope
(~20-60 min)
- Reconstruct images of
radiotracer distribution
(nCi/cc)
6
+
+ +
NucleusNucleus
NeutronsNeutrons
ProtonsProtons
ElectronsElectrons
Positron (Positron (ββ++
) Decay) Decay
18
F-FDG
7
ββ++
DecayDecay
+
+
+
+
+
+
+
+
+
Neutron-deficient isotopes can decay by emittingNeutron-deficient isotopes can decay by emitting
positronspositrons
+
anti-neutrinoanti-neutrino
positronpositron Net effect: oneNet effect: one
protonproton
replaced byreplaced by
• neutronneutron
• anti-neutrinoanti-neutrino
• positronpositron
8
Positron annihilation
Annihilation gives
• 2x 511 keV gamma rays
• 180 degrees apart
• Line of response
Positron range & gamma
noncollinearity
Scanner is just a photon
counter!
• Counts gamma-ray pairs vs.
single gammas
• Time window ~ 1 ns
511 keV
511 keV
e+
e-
9
Raw Data & Image Reconstruction
0° projection
0°
180°
90°
90°projection
image
reconstruction
“sinogram”
10
Important Detector PropertiesImportant Detector Properties
- Spatial resolution
- Directly controls spatial resolution
in reconstructed image
- Currently ~ 1 - 5 mm
- Depth-of-interaction?
- Reduces “parallax”
11
Important Detector PropertiesImportant Detector Properties
- Detection efficiency (aka sensitivity, stopping power)
- Reduces noise from counting statistics
- Currently > ~ 30% (singles)
55M Events1M Events
12
Important Detector PropertiesImportant Detector Properties
Random (accidental) coincidence
- Time resolution
- Affects acceptance of random
coincidences
- Currently ~ 1 - 10 ns
- Time-of-flight (TOF)?
- c = ~ 1 ft/ns
- Need << 1 ns resolution
13
Important Detector PropertiesImportant Detector Properties
Scatter and Attenuation
511 keV
- Energy resolution
- Scattered gammas change
direction AND lose energy
- Affects acceptance of scattered
coincidences
- Currently ~ 20%
- Deadtime
- Handle MHz count rates!
511 keV 400 keV
14
Scintillation
Crystal
PMT
Pre-Amplifier
+ Electronics
Gamma photon
converts to optical
photons
(proportional to
gamma energy, typ.
1000’s)
photons are
collected at the end
of the crystal
light is converted to an electrical signal
& amplified
Front-end electronics
condition the signal for
further processing
Prototypical PET Detector
Gamma Ray
Optical reflector
15
New Developments
• Detectors
• Multimodality imaging
• Specialized applications
16
Scintillator NaI(Tl) BGO GSO LSO LuAP LPS LaBr
τ (ns) 230 300 60 40 18 30 35
µ (cm-1
) 0.35 0.95 0.70 0.86 0.95 0.70 0.47
∆E/E (%) 6.6 10.2 8.5 10.0 ~15 ~10 2.9
Rel. light output (%) 100 15 25 70 30 73 150175
25
New Developments: Detectors
• Scintillators
• No perfect choice - tradeoffs
• Also practical qualities
• Rugged?
• Hygroscopic?
• Cost?
17
New Developments: Detectors
• Photosensors
• Photomultiplier tubes
• Avalanche photodiodes
• Arrays, position-sensitive
• Compact but noisier
• Silicon photomultipliers
• Very new
• Best of both?
APD array
PMT
SiPM
18
New Developments: Detectors
• Solid-state
detectors
• Direct conversion,
no photodetector
• Great dE/E &
spatial resolution
• Poorer timing &
stopping power
• CZT Z2
Z1
Sa2
Sa1
Sc
⊕
∅
⊕
⊕
∅
∅
⊕
∅
19
New Developments: Detectors
• Pb converters & ionization
HIDAC Pb-walled straws (50 cm long)
20
New Developments: Detectors
• 3D gamma-ray event positioning
• Depth of interaction
• Reduces parallax problem
LSO
slab
γ γ
APD
slab
s
vs.
LSO slab
crystal
holder
APD
decoupling
capacitor
HV filter
capacitor
Current-
limiting
resistor
signal
output
connector
SHV
connector
unused APD
slot
21
New Developments: Detectors
• Time of flight using LaBr3
noTOF300psTOF
1 Mcts 5 Mcts 10 Mcts
22
New Developments
• Multimodality imaging
• PET/CT
• PET/MRI
• Specialized applications
• Brain, breast, prostate
• Small animal - microPET
• Arterial input function
• Humans - wrist scanner
• Animals - microprobe
• Awake rat brain - RatCAP
23
RatCAP: Rat Conscious Animal PET
Eliminate anesthesia in preclinical neuroscience
using PET in order to:
• Remove confounding effects of anesthetic on
neurochemistry
• Enable stimulation in animal PET
• Enable correlations of behavior and neuro-PET
24
Architecture
Detector blocks x12
• LSO 2.2 x 2.2 x 5 mm in 4 x 8 array
• 1:1 coupling to APD
• ASIC - single all digital output
Timestamp & Signal Processing Module
• Programmable real-time logic (FPGA)
• 1 ns bins (debugging, now 10 ns)
Data acquisition
• PCI card in standard PC
• Up to 70 MB/s = ~10 Mcps singles
• Offline software for coincidences, corrections, recon, …
TSPM
TDC
PCI
card
ASIC
opticaldifferential
RatCAP
25
Architecture
RatCAP
TSPM
LSO APD
ASICs
all interconnections
38 mm FOV
72 mm OD optical links to PCI
high voltage
194 g
data, clock, power
18mmaxialFOV
26
Performance
Spatial resolution (FWHM @ CFOV)
• FBP: 2.1 mm
• MLEM: <1.5 mm
Energy resolution: 23% FWHM
Time resolution: 14 ns FWHM
• window = 30 ns
Sensitivity (point @ CFOV): 0.7%
Peak Noise Equivalent Count rate: 14 kcps @ 5 µCi/cc
1st prototype: LLD = 150 keV average, variable
27
Imaging Conditions
Anesthetized 250-350 g rats
Limited DAQ livetime >> long scans for statistics
Artifacts
28
F-18 Fluoride Bone Scan
1.3 mCi fluoride
RatCAP microPET R4
29
C-11 Raclopride
1.8 mCi raclopride
In the RatCAP
30
C-11 Methamphetamine
Time-activity curve for striatum
31
Thanks!
DOE OBER funding

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Nuc chemsummerschool 072106-v2

  • 1. 1 Physics & Instrumentation in Positron Emission Tomography Paul Vaska, Ph.D. Center for Translational Neuroscience Brookhaven National Laboratory July 21, 2006
  • 2. 2 Non-invasive Medical Imaging Techniques Anatomical • X-ray • CAT • MRI • Ultrasound Functional • “nuclear medicine” - SPECT, PET CAT X-Ray MRI
  • 3. 3 Positron Emission Tomography Recent mainstream acceptance - relatively expensive - cyclotron for tracer production - detectors must stop high-energy gamma-rays - low resolution (>2 mm), limited counting statistics - BUT unique functional capabilities Applications - Diagnosis of disease - cancer (WB), cardiac, … - Research - brain function - animal studies
  • 4. 4 Technical Challenges in PET Imaging Radiochemistry - better tracers Imaging Physics - better images by • Detector design – Spatial resolution – Sensitivity • Image processing – Corrections for physical effects – Image reconstruction algorithms Data Analysis & Biological Modeling - better interpretation of images
  • 5. 5 PET Imaging Overview - Synthesize radiotracer - Inject radiotracer - Measure gamma-ray emissions from isotope (~20-60 min) - Reconstruct images of radiotracer distribution (nCi/cc)
  • 7. 7 ββ++ DecayDecay + + + + + + + + + Neutron-deficient isotopes can decay by emittingNeutron-deficient isotopes can decay by emitting positronspositrons + anti-neutrinoanti-neutrino positronpositron Net effect: oneNet effect: one protonproton replaced byreplaced by • neutronneutron • anti-neutrinoanti-neutrino • positronpositron
  • 8. 8 Positron annihilation Annihilation gives • 2x 511 keV gamma rays • 180 degrees apart • Line of response Positron range & gamma noncollinearity Scanner is just a photon counter! • Counts gamma-ray pairs vs. single gammas • Time window ~ 1 ns 511 keV 511 keV e+ e-
  • 9. 9 Raw Data & Image Reconstruction 0° projection 0° 180° 90° 90°projection image reconstruction “sinogram”
  • 10. 10 Important Detector PropertiesImportant Detector Properties - Spatial resolution - Directly controls spatial resolution in reconstructed image - Currently ~ 1 - 5 mm - Depth-of-interaction? - Reduces “parallax”
  • 11. 11 Important Detector PropertiesImportant Detector Properties - Detection efficiency (aka sensitivity, stopping power) - Reduces noise from counting statistics - Currently > ~ 30% (singles) 55M Events1M Events
  • 12. 12 Important Detector PropertiesImportant Detector Properties Random (accidental) coincidence - Time resolution - Affects acceptance of random coincidences - Currently ~ 1 - 10 ns - Time-of-flight (TOF)? - c = ~ 1 ft/ns - Need << 1 ns resolution
  • 13. 13 Important Detector PropertiesImportant Detector Properties Scatter and Attenuation 511 keV - Energy resolution - Scattered gammas change direction AND lose energy - Affects acceptance of scattered coincidences - Currently ~ 20% - Deadtime - Handle MHz count rates! 511 keV 400 keV
  • 14. 14 Scintillation Crystal PMT Pre-Amplifier + Electronics Gamma photon converts to optical photons (proportional to gamma energy, typ. 1000’s) photons are collected at the end of the crystal light is converted to an electrical signal & amplified Front-end electronics condition the signal for further processing Prototypical PET Detector Gamma Ray Optical reflector
  • 15. 15 New Developments • Detectors • Multimodality imaging • Specialized applications
  • 16. 16 Scintillator NaI(Tl) BGO GSO LSO LuAP LPS LaBr τ (ns) 230 300 60 40 18 30 35 µ (cm-1 ) 0.35 0.95 0.70 0.86 0.95 0.70 0.47 ∆E/E (%) 6.6 10.2 8.5 10.0 ~15 ~10 2.9 Rel. light output (%) 100 15 25 70 30 73 150175 25 New Developments: Detectors • Scintillators • No perfect choice - tradeoffs • Also practical qualities • Rugged? • Hygroscopic? • Cost?
  • 17. 17 New Developments: Detectors • Photosensors • Photomultiplier tubes • Avalanche photodiodes • Arrays, position-sensitive • Compact but noisier • Silicon photomultipliers • Very new • Best of both? APD array PMT SiPM
  • 18. 18 New Developments: Detectors • Solid-state detectors • Direct conversion, no photodetector • Great dE/E & spatial resolution • Poorer timing & stopping power • CZT Z2 Z1 Sa2 Sa1 Sc ⊕ ∅ ⊕ ⊕ ∅ ∅ ⊕ ∅
  • 19. 19 New Developments: Detectors • Pb converters & ionization HIDAC Pb-walled straws (50 cm long)
  • 20. 20 New Developments: Detectors • 3D gamma-ray event positioning • Depth of interaction • Reduces parallax problem LSO slab γ γ APD slab s vs. LSO slab crystal holder APD decoupling capacitor HV filter capacitor Current- limiting resistor signal output connector SHV connector unused APD slot
  • 21. 21 New Developments: Detectors • Time of flight using LaBr3 noTOF300psTOF 1 Mcts 5 Mcts 10 Mcts
  • 22. 22 New Developments • Multimodality imaging • PET/CT • PET/MRI • Specialized applications • Brain, breast, prostate • Small animal - microPET • Arterial input function • Humans - wrist scanner • Animals - microprobe • Awake rat brain - RatCAP
  • 23. 23 RatCAP: Rat Conscious Animal PET Eliminate anesthesia in preclinical neuroscience using PET in order to: • Remove confounding effects of anesthetic on neurochemistry • Enable stimulation in animal PET • Enable correlations of behavior and neuro-PET
  • 24. 24 Architecture Detector blocks x12 • LSO 2.2 x 2.2 x 5 mm in 4 x 8 array • 1:1 coupling to APD • ASIC - single all digital output Timestamp & Signal Processing Module • Programmable real-time logic (FPGA) • 1 ns bins (debugging, now 10 ns) Data acquisition • PCI card in standard PC • Up to 70 MB/s = ~10 Mcps singles • Offline software for coincidences, corrections, recon, … TSPM TDC PCI card ASIC opticaldifferential RatCAP
  • 25. 25 Architecture RatCAP TSPM LSO APD ASICs all interconnections 38 mm FOV 72 mm OD optical links to PCI high voltage 194 g data, clock, power 18mmaxialFOV
  • 26. 26 Performance Spatial resolution (FWHM @ CFOV) • FBP: 2.1 mm • MLEM: <1.5 mm Energy resolution: 23% FWHM Time resolution: 14 ns FWHM • window = 30 ns Sensitivity (point @ CFOV): 0.7% Peak Noise Equivalent Count rate: 14 kcps @ 5 µCi/cc 1st prototype: LLD = 150 keV average, variable
  • 27. 27 Imaging Conditions Anesthetized 250-350 g rats Limited DAQ livetime >> long scans for statistics Artifacts
  • 28. 28 F-18 Fluoride Bone Scan 1.3 mCi fluoride RatCAP microPET R4
  • 29. 29 C-11 Raclopride 1.8 mCi raclopride In the RatCAP