PET Quantification Flashcards

1
Q

Why is quantification theoretically possible in PET and not in SPECT?

A

The attenuation along a known line of response is independent of the unknown position of the emission along that line.

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2
Q

What is the purpose of quantification of PET?

A
  • Lesion characterisation
  • Response assessment
  • Data reduction in trials & statistical analysis
  • Dose optimisation/response assessment
  • Testing drug targeting
  • Radiotherapy target identification – functional target volumes with
    reduced inter-observer variability
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3
Q

What are the types of corrections and calibrations required to calculate the activity concentration? (6)

A
  • Randoms Correction
  • Normalisation
  • Dead Time Correction
  • Scatter Correction
  • Attenuation Correction
  • PET Scanner Calibration
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4
Q

What are ‘Randoms’?

A

Randoms arise when two uncorrelated single detection events happen with sufficient temporal proximity to fall within the trues detection window. They can be estimated from singles count rates.

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5
Q

What is the singles count rate equation?

A

C_ij = 2 x τ x r_i x r_j

Where Cij is the rate (randoms per second) of random coincidences along line of response Lij, which connects detectors at channel i and j. ri and rj are the singles rates at these channels respectively and τ is the timing window for coincidences.

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6
Q

What are the different types of randoms corrections? (3)

A
  1. Estimation from singles rates - simply integrate the expression for randoms rate over the acquisition time T.
  2. Delayed coincidence channel - A duplicate window is set up at a delay from the coincidence window, but is open for the same time and exposed to the same dead time conditions etc as the coincidence window. This removes the correlated events (true coincidences), but gives an accurate rate of the randoms component
  3. Tailfitting - looking at distribution of random coincidences at the edges of the sinogram
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7
Q

What is the purpose of normalisation?

A

To compensate for variable sensitivities.

An individual correction factor is required for each line of response in the scanner.

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8
Q

What are the causes of variable sensitivity? (6)

Think of the Normalisation Equation

A
  • Axial data summing and “mashing”
  • Detector Efficiency
  • Geometric & Solid angle effects
  • Time window alignment
  • Structural alignment
  • Septa
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9
Q

What are the reasosn for detector efficiency variation?

A
  • Position within the block; this is systematic and predictable and is called the
    “block profile”.
  • Physical differences in the crystal and light guide
  • PM tube gains varying

The latter two should be familiar from sensitivity map corrections of gamma cameras.

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10
Q

What are the geometric and solid angle effects?

A

These effects occur as lines of response are narrower closer to the edge of the field of view. The position and angle of incidence of the incoming photon affects the depth of mateiral along its path and hence the probability of interaction causing varying detection efficiencies. Reducing acceptance angles which causes a reduction in sensitivity.

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11
Q

How do you mitigate geometric and solid angle effects?

A

The effects are calculated analytically and incorporated into the recontruction algorithms, termed the ‘arc correction’.

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12
Q

What is the purpose of time window alignment?

A

Important for coincidence timing to be accurately synchronised.
Asychronicity offsets the coincidence window which reduces sensitivity to true coincidences, but not the
number or random events detected

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13
Q
A
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14
Q

What is the effect of minor structural misalignment of the modules in the ring system?

A

They affect the sensitivity of the lines of response.

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15
Q

Describe the method of direct normalisation?

A
  • Illuminating all possible lines of response using a positron source
  • An analytical correction is made for non-unifrom radial illumination
  • Normalisation coefficients combining all the effects are taken to be inversely proportional to the counts acquired in each LOR

Positron source typically used is 68Ge

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16
Q

What are the problems with direct normalisation? (3)

A
  1. Long aquisitions
  2. Dependant on excellent source uniformity
  3. Scatter isnt comparable to patient scatter which can cause artefacts and bias
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17
Q

What causes a finite chance of counts occurring within the minimum time window of PET systems?

A

The random nature of radioactive decay causes a finite chance of counts occurring within this window, even at low activity levels.

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18
Q

How does higher activity affect the detection accuracy in PET scanners?

A

At higher activity levels, the chance of overlapping counts increases, leading to greater effects of system limitations.

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19
Q

What is fractional dead time, and how is it defined?

A

Fractional dead time is the ratio of measured count rate to the expected count rate at a given activity level.

20
Q

Why are corrections necessary for accurate quantification in PET imaging?

A

Actual count rates are not directly proportional to the number of positron decays, so corrections are needed for accuracy across various activity concentrations.

21
Q

How can dead time be measured in PET imaging?

A

Dead time can be measured using a decaying source experiment.

22
Q

How are expected count rates determined in dead time correction?

A

Expected rates are obtained by extrapolating from very low count data, where dead time effects are negligible.

23
Q

What is the simplest method for dead time correction? And what is the issue with this method?

A

The simplest corrections use results from experiments to create lookup tables for correction factors.

BUT simple look up tables ignore spatial variations in source distribution and so the chosen factor is unlikely to be relevant to all the subsystems to which it is being applied.

24
Q

What is a more sophisticated method for dead time correction?

A

More accurate approaches measure or model the “live time” of each sub-system, calculated as:
Live time = Acquisition time x (1 - fractional dead time).

25
Q

What are the components of system dead time?

A

System dead time consists of “paralysable” and “non-paralysable” components.

26
Q

At 511 keV what is the most likely interaction to occur within the body?

A

Compton Scatter

27
Q

Why is scatter challenging to exclude in PET scanners?

A
  • The Compton equation shows a photon can scatter up to 45° while losing only 115 keV of energy to the recoil electron.
  • PET scanners have poor energy resolution, with wide acceptance windows (e.g., 350–650 keV), making it difficult to effectively exclude scatter.
28
Q

What is scatter fraction?

A

Scatter fraction is the proportion of accepted coincidences that have undergone Compton Scattering. Typically ~15% for a 2D scanner ~40% in a 3D scanner

29
Q

What does the scatter fraction depend on?

A
  • 2D or 3D scanner design
  • Energy window
  • Size of the scattering medium
  • Density of the scattering medium
30
Q

What are the behaviours of scatter in PET imaging, and how is it handled?

A
  • LORs outside the object boundary (post-randoms correction) are exclusively scatter.
  • Scatter distribution is broad, containing low spatial frequency data.
  • The coincidence energy spectrum includes a large scatter component, but it is not exclusively scatter due to limited energy resolution.
  • Scattered coincidences within the energy window are mostly from singly scattered paths.
  • These features are used for scatter estimation and correction methods.
31
Q

What are the types of scatter correction?

A
  • Fitting scatter tails
  • Direct Measurement (only applicable to scanners with retractable septa)
  • Multiple energy window techniques
  • Convolution and Deconvolution approaches
  • Analytical Simulation
  • Monte Carlo Simulation
32
Q

What is the equation for attenuation correction?

A

C=C0e(-μD)

Where D is the total distance through the body.

33
Q

Describe the components in the equation for attenuation correction?

A

C = measured counts
C0 = attenuation corrected counts
D = the total thickness through the body
μ = attenuation coefficient

34
Q

How is the attenuation coefficient determined?

A

Houndsfeld units describing CT attenuation are mapped to estimate attenuation coefficients for 511keV annihilation photons

35
Q

What are the challenges of attenuation correction in PET imaging?

A
  • Implants and CT artifacts can cause inaccuracies in attenuation maps.
  • Scanning in certain positions (e.g., arms down or treatment planning) may require extended fields of view, leading to truncation and estimation errors in attenuation maps.
  • PET-MR scanning lacks direct attenuation information, requiring specialized sequences and segmentation methods for estimation.
36
Q

What causes partial volume effects in PET imaging, and what are their impacts?

A
  • Partial volume effects occur due to PET’s finite spatial resolution and limited spatial sampling frequency.
  • Activity concentrations in small structures are underestimated because activity is spread over a larger volume than the structure itself.
  • This reduces contrast for qualitative review and underestimates activity concentration for quantitation.
37
Q

Why is calibration important in PET imaging, and how is it performed?

A
  • Calibration ensures the scanner references absolute activity concentrations.
  • Typically, a cross-calibration with a traceably calibrated dose calibrator is performed to maintain consistency in activity measurements for SUV calculations.
  • In facilities with multiple calibrators, all must agree within tight tolerances or maintain a one-to-one relationship with the scanner.
  • Cross-calibration is also required for equipment used in blood counting or other analysis steps.
38
Q

What factors can impact quantification in PET imaging, even with an optimal scanner setup?

A
  • Metabolites
  • ROI definition
  • Partial volume effect
  • Heterogeneity
  • Movement correction
39
Q

What is the equation for the Standard Uptake Value?

A

SUV = Activity Concentration/ (Injected Dose/Body Weight)

40
Q

What are the common methods for calculating Body Weight in PET imaging?

A

A. Body Mass
* Most common and straightforward.

B. Lean Body Mass
* More complex; choice of measurement or estimation technique is critical.
* More consistent across different body types for FDG, as fat has very low uptake.

C. Body Surface Area
* Tallies with some dosing regimes.

41
Q

What are the definitions of SUVmax, SUVmean, and SUVpeak in PET imaging?

A

**SUVmax: **The maximum standardized uptake value in a region of interest (ROI).
SUVmean: The average standardized uptake value across all voxels in the ROI.
SUVpeak: The average standardized uptake value in a small, user-defined subregion around the highest activity, balancing precision and noise.

42
Q

What is the correction of FDG SUV for blood gucose level?

A

x Glucoseplasma(mmol/l)/5.0 (mmol/l)

43
Q

What are common errors affecting SUV (Standardized Uptake Value) in PET imaging, and their impacts?

A

Incorrect cross-calibration: Causes a systematic SUV error equal to the relative cross-calibration error.
**Residual activity in administration system: ** Reduces net administered dose, leading to underestimated SUVs.
**Incorrect decay correction: ** Results in incorrect SUV values.
Tissued injection: May lead to inaccurate SUV due to improper tracer delivery.

44
Q

What clinical and patient factors affect the accuracy and reproducibility of SUV in PET imaging?

A

Blood glucose level: Higher blood glucose reduces FDG uptake, leading to lower SUV.
Uptake period: Imaging at different points on the uptake curve can result in varying SUV values.
Patient comfort: Discomfort increases FDG uptake in brown fat and muscles, potentially lowering SUV elsewhere or causing spillover of counts into adjacent lesions.
Inflammation: Inflammation can cause false positives, leading to increased SUV.
Patient motion/breathing: Mismatched attenuation correction and motion artifacts can blur counts, potentially lowering the SUV estimate.

45
Q
A