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Synergies Between Calorimetry and PETSynergies Between Calorimetry and PET
William W. MosesLawrence Berkeley National Laboratory
March 26, 2002
Outline:– Fundamentals of PET
– Comparison of Calorimetry & PET
– Areas of Common Interest
– Conclusions
Step 1: Inject Patient with Radioactive DrugStep 1: Inject Patient with Radioactive Drug
• Drug is labeled with positron(+) emitting radionuclide.
• Drug localizes in patient according to metabolic properties of that drug.
• Trace (pico-molar) quantities of drug are sufficient.
• Radiation dose fairly small(<1 rem).
Drug Distributes in BodyDrug Distributes in BodyDrug Distributes in BodyDrug Distributes in Body
Ideal Tracer IsotopeIdeal Tracer Isotope
18F 2 hour half-life15O, 11C, 13N 2, 20, & 10 minute half-lives
18F 2 hour half-life15O, 11C, 13N 2, 20, & 10 minute half-lives
• Interesting BiochemistryEasily incorporated into biologically active drugs.
• 1 Hour Half-LifeMaximum study duration is 2 hours.Gives enough time to do the chemistry.
• Easily ProducedShort half life local production.
Step 2: Detect Radioactive DecaysStep 2: Detect Radioactive DecaysRing of PhotonDetectors
• Radionuclide decays, emitting +.
+ annihilates with e– from tissue, forming back-to-back 511 keV photon pair.
• 511 keV photon pairs detected via time coincidence.
• Positron lies on line defined by detector pair (known as a chord or a line of response or a LOR).
Detect Pairs of Back-to-Back 511 keV PhotonsDetect Pairs of Back-to-Back 511 keV Photons
Multi-Layer PET CamerasMulti-Layer PET Cameras
• Can image several slices simultaneously• Can image cross-plane slices• Can remove septa to increase efficiency (“3-D PET”)
Planar Images “Stacked” to Form 3-D ImagePlanar Images “Stacked” to Form 3-D Image
Scintillator Tungsten Septum Lead Shield
Step 3: Reconstruct with Computed Tomography
Step 3: Reconstruct with Computed Tomography
2-Dimensional Object
By measuring all 1-dimensional projections of a2-dimensional object, you can reconstruct the object
By measuring all 1-dimensional projections of a2-dimensional object, you can reconstruct the object
1-Dimensional Vertical Projection
1-Dimensional Horizontal Projection
Why Do Computed Tomography?Why Do Computed Tomography?
Planar X-Ray Computed Tomography
Images courtesy of Robert McGee, Ford Motor Company
Separates Objects on Different PlanesSeparates Objects on Different Planes
Attenuation CorrectionAttenuation Correction
• Use external + source to measure attenuation.
• Attenuation (for that chord) same as for internal source.
• Source orbits around patient to measure all chords.
• Measure Attenuation Coefficient for Each Chord• Obtain Quantitative Images
• Measure Attenuation Coefficient for Each Chord• Obtain Quantitative Images
+ Source
Time-of-Flight TomographTime-of-Flight Tomograph
• Can localize source along line of flight.
• Time of flight information reduces noise in images.
• Time of flight tomographs have been built with BaF2 and CsF.
• These scintillators force other tradeoffs that reduce performance.
c = 1 foot/ns500 ps timing resolution 8 cm fwhm localization
Not Compelling with Present Technology...Not Compelling with Present Technology...
NMR & PET Images of EpilepsyNMR & PET Images of Epilepsy
• NMR “Sees” Structure with 0.5 mm Resolution
• PET “Sees” Metabolism with 5.0 mm Resolution
NMR PET
PET Images of CancerPET Images of Cancer
Metastases Shown with Red Arrows
Brain Heart
Bladder
Normal Uptake in Other Organs Shown in Blue
Treated Tumor Growing Again on
Periphery
PET Camera DesignPET Camera Design
• Typical Parameters
• Detector Module Design
PET CamerasPET Cameras
• Patient port ~60 cm diameter.• 24 to 48 layers, covering 15 cm axially.• 4–5 mm fwhm spatial resolution.• ~2% solid angle coverage.• $1 – $2 million dollars.
Images courtesy of GE Medical Systems and Siemens / CTI PET Systems
Early PET Detector ElementEarly PET Detector Element
BGO Scintillator Crystal(Converts into Light)
Photomultiplier Tube(Converts Lightto Electricity)
3 — 10 mm wide(determines in-plane
spatial resolution)
10 — 30 mm high(determines axialspatial resolution)
30 mm deep(3 attenuation
lengths)
Modern PET Detector ModuleModern PET Detector Module
BGO Scintillator Crystal Block(sawed into 8x8 array,
each crystal 6 mm square)
4 PMTs(25 mm square)
50 mm
50 mm30 mm
• Saw cuts direct light toward PMTs.
• Depth of cut determines light spread at PMTs.
• Crystal of interaction found with Anger logic (i.e. PMT light ratio).
Good Performance, Inexpensive, Easy to PackGood Performance, Inexpensive, Easy to Pack
Crystal Identification with Anger LogicCrystal Identification with Anger Logic
0500
1000150020002500300035004000
Counts
Can Decode Up To 64 Crystals with BGOCan Decode Up To 64 Crystals with BGOX-Ratio
Y-Ratio
Uniformly illuminate block.
For each event, computeX-Ratio and Y-Ratio,then plot 2-D position.
Individual crystals show up as dark regions.
Profile shows overlap (i.e. identification not perfect).
ProfilethroughRow 2
Fundamental Limits of Spatial ResolutionFundamental Limits of Spatial Resolution
• Dominant Factor is Crystal Width• Limit for 80 cm Ring w/ Block Detectors is 3.6 mm
• Dominant Factor is Crystal Width• Limit for 80 cm Ring w/ Block Detectors is 3.6 mm
d/2
Reconstruction Algorithm1.25 (in-plane)1.0 (axial)
Factor
d
Detector Crystal Width
Photon Noncollinearity
180° ± 0.25°
Positron Range
Shape FWHM
multiplicative factor
0.5 mm (18F)4.5 mm (82Rb)
1.3 mm (head)1.8 mm (heart)
0 (individual coupling)2.2 mm (Anger logic)* *empirically determined from published data
Anger Logic
Tangential Projection
Radial ElongationRadial Elongation
• Penetration of 511 keV photons into crystal ring blurs measured position.
• Effect variously known as Radial Elongation, Parallax Error, or Radial Astigmatism.
• Can be removed by measuring depth of interaction.Radial
Projection
PET Front End ElectronicsPET Front End Electronics
AnalogASIC
Custom ASIC
PMT APMT BPMT CPMT D
EnergyADC
FPGAX
ADCY
ADCTime
TDC
RAM
Off the Shelf
“Singles”Event Word
• Position• Time
• Digitize Arrival Time (latch 500 MHz clock — 2 ns accuracy)• Identify Crystal of Interaction & Measure Energy• Correct Energy and Arrival Time (based on crystal)• Maximum “Singles” Event Rate is 1 MHz / Detector Module
If Energy Consistent with 511 keV,Send Out “Singles” Event Word (Position & Time)
If Energy Consistent with 511 keV,Send Out “Singles” Event Word (Position & Time)
PET Readout ElectronicsPET Readout Electronics
FPGAsFiber Optic
Interface
Off the Shelf
“Coincidence”Event Word
• Locationof Chord
Singles 0
• Search for “Singles” in Time Coincidence (~10 ns window)• Strip Off Timing Information• Format “Coincidence” Event Word (chord location)• Maximum “Coincidence” Event Rate is 10 MHz / Camera
Search for Coincidences, Send Out “Coincidence” Event Word (Position of Chord)
Search for Coincidences, Send Out “Coincidence” Event Word (Position of Chord)
Singles n
.
.
.
From Each Camera Sector
Similarities and DifferencesBetween Calorimetry & PETSimilarities and DifferencesBetween Calorimetry & PET
• Similarities
• The PET World Picture...
Similarities Between Calorimeters and PETSimilarities Between Calorimeters and PET
PET CameraCalorimeter
• Cylindrical Gamma Ray Detectors• High Efficiency, Hermetic• Segmented, High Density Scintillator Crystals• High Performance Photodetectors• High Rate, Parallel Readout Electronics
The PET World Picture:The PET World Picture:
Signal Levels Are Very LowSignal Levels Are Very Low
*511 keV
Need to Image
0.000000511 TeV*Photons
No Pair Production / EM ShowersNo Pair Production / EM Showers
• Compton scatter in patient produces erroneous coincidence events.
• ~15% of detected events are scattered in 2-D PET(i.e. if tungsten septa used).
• ~50% of events are scatteredin 3-D Whole Body PET.
• Compton Scatter is Important Background• Use Energy to Reject Scatter in Patient
• Compton Scatter is Important Background• Use Energy to Reject Scatter in Patient
Scatter Length ≈ 10 cm
Patient Radiation Dose is Limited!Patient Radiation Dose is Limited!
• Cannot Increase Signal Source Strength• Image Noise Is Limited by Counting Statistics
• Cannot Increase Signal Source Strength• Image Noise Is Limited by Counting Statistics
Competitive Commercial MarketCompetitive Commercial Market
Cost is Very ImportantCost is Very Important
• $60 Million (parts cost)
• 72,000 Channels
• $833 / Channel
• $1 Million (parts cost)
• 18,400 Channels
• $54 / Channel
CMS Calorimeter PET Camera
• Scintillator crystals are ~25% of total parts cost
• Photomultiplier tubes are ~25% of total parts cost
• No other component is >10% of total parts cost
In a PET Camera:
PET Detector RequirementsPET Detector Requirements
Detect 511 keV Photons With(in order of importance):
• >85% efficiency
• <5 mm spatial resolution
• “low” cost (<$100 / cm2)
• “low” dead time (<1 µs cm2)
• <5 ns fwhm timing resolution
• <100 keV fwhm energy resolution
Based on Current PET Detector ModulesBased on Current PET Detector Modules
Synergies...Synergies...
• Scintillators
• Photodetectors
• Electronics
• Computation
Very Strong Parallels...Very Strong Parallels...
New Scintillators Developed RecentlyNew Scintillators Developed Recently
Image courtesy of E. Auffray, CERN
LSOPbWO4
Image courtesy of C. Melcher, CTI PET Systems
• Discovered in ~1992.• Approximately 10 years of R&D before large scale production.• Development efforts driven by end users, but included efforts
of luminescence scientists, spectroscopists, defects scientists, materials scientists, and crystal growers.
Scintillator PropertiesScintillator Properties
Different Tradeoffs RequiredDifferent Tradeoffs Required
PbWO4
Lu2SiO5
Density (g/cc): 8.3 7.4
Attenuation Length (cm): 0.9 1.2
Light Output (phot/MeV): 200 25,000
Decay Time (ns): 10 40
Emission Wavelength (nm): 420 420
Radiation Hardness (Mrad): >10 10
Dopants: Y, Nd Ce
Cost per cc: $1 >$25
Avalanche Photodiode ArraysAvalanche Photodiode Arrays
RMD, Inc.Hamamatsu Photonics
Advantages:• High Quantum Efficiency Energy Resolution• Smaller Pixels Spatial Resolution• Individual Coupling Spatial Resolution
Challenges:• Dead Area Around Perimeter• Signal to Noise Ratio• Reliability and Cost
APD RequirementsAPD Requirements
Calorimetry PET
High Gain?: Yes Yes
High QE / Blue Sensitivity?: Yes Yes
Radiation Hardness?: Yes No
Nuclear Counter Effect?: Yes No
Timing Signal (low C)?: No Yes
High Packing Density?: No Yes
Sensitive to Leakage Current?: ~ Yes
Different Tradeoffs RequiredDifferent Tradeoffs Required
Electronics RequirementsElectronics Requirements
Calorimetry PET
Low Noise Analog Amplifier?: Yes Yes
Low Power Consumption?: Yes Yes
Mixed-Mode Custom ICs?: Yes Yes
Real-Time Data Correction?: Yes Yes
Highly Parallel Readout?: Yes Yes
High Data Rate?: Yes Yes
Many SimilaritiesMany Similarities
Electronics RequirementsElectronics Requirements
Calorimetry PET
Radiation Damage?: Yes No
Analog Dynamic Range: High Low
Self-Generated Timing Signal?: No Yes
Asynchronous Inputs?: No Yes
Event Size / Complexity?: High Low
Multiple Trigger Levels?: Yes No
“Good” Event Rate?: kHz MHz
Different Tradeoffs RequiredDifferent Tradeoffs Required
Computation RequirementsComputation Requirements
Calorimetry PET
Significant Computation?: Yes Yes
Monte Carlo Simulation?: Yes Yes
Large Programming Project?: Yes Yes
Complexity of Analysis?: High Low
Data Set Size?: TB–PB GB
Time to Finish Analysis?: YearsMinutes
FDA Certification Required?: No YesDifferent Tradeoffs RequiredDifferent Tradeoffs Required
Final ThoughtsFinal Thoughts
Many Synergies Exist Between HEP & PETScintillators, detectors, electronics, computing, …
Tools & experience are particularly valuable
PET is a Mature, Commercial Technology Innovations will only be used if they are
clearly superior (not just novel) All requirements must be met Cost is very important
Difficult to Transfer Identical TechnologyNeed to optimize for PET tradeoffs