Topic 13: PET & SPECT Flashcards

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1
Q

What is SPECT?

A

Single photon emission (computed) tomography, substance labelled with radio-nuclide (photon emission), relatively cheap but relatively low resolution and sensitivity

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2
Q

What is PET?

A

Positron emission tomography, substance labelled with radio-nuclide (positron emission), expensive due to scanner and cyclotron.

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3
Q

Two other functional tomographic modalities other than PET and SPECT?

A

MRI spectroscopy and functional MRI.

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4
Q

Radionuclides used in SPECT?

A

Technetium-99m, Thallium-201

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5
Q

Example clinical applications of SPECT?

A

Cardiac perfusion, parkinson’s and blood flow.

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6
Q

Positron Emission Tomography

A

Substance labelled with radio-nuclide. Radioactive decay is a random process Detection of photon-pair, no collimator necessary,

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7
Q

PET physics mechanism?

A

An unstable nucleus emits a positron and a neutrino and the positron hits an electron, and 2 gamma photons are emitted in opposite directions. The two gamma photons are detected at the same time in the detector, with a slight difference (we call this a timing window then we call it a coincidence)

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8
Q

PET applications in medicine?

A

oncology (cancer) neurology psychiatry cardiology What for? - diagnosis, measuring therapy effectiveness and drug development.

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9
Q

The advantage of PET?

A

Sensitive for picomolar concentrations.

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10
Q

What factors influence quality of the PET image?

A

-Biology - Scanner - amount of detected counts - Image reconstruction and processing (including kinetic modelling algorithms)

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11
Q

poisson noise process variance and CV calculations?

A

variance = mean CV = STD/MEAN=1/SQRT(MEAN)

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12
Q

if we have more counts what does that mean for noise?

A

so cv is lower for higher mean. so for more counts we will be happier as we will have less noise.

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13
Q

activity

A

(average) rate of emissions/decays

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14
Q

how do you relate half life and lambda?

A

lambda = ln(2)/half-life

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15
Q

what is the decay of radioactive decay?

A

1-exp(-lamba*Time)

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16
Q

the number of decays in time interval [0,T] is _____ distributed.

A

Poisson distributed

17
Q

what is the mean of counts that are poisson distributed?

A
18
Q

what is the coefficient of variation for counts with a poisson distribution?

A

1/sqrt (mean of counts)

19
Q

How do you increase counts?

A

1) Inject more radioactivity
- Limitations;

patient dose, scanner counting limitations, purity of inject substance

2) Scan longer

limitation:

scanning time available, patient movement

3) Avoid attenuation

limitations:

patient comfort

20
Q

What is the LOR?

A

Each coincidence event represents a line in space connecting the two detectors along which the positron emission occurred (i.e., the line of response (LOR)).

21
Q

the mean number of _____ ____ will therefore be proportional to the accumulated acitivity on that LOR.

A

Detected events

22
Q

Two different reconstruction algorithms?

A

Anlaytic e.g. filter back projection or

statistical e.g. maximum likelihood.

23
Q

What are analytic methods?

A

They are based on mathematical inversion of the complete set of ‘line integrals’ (X-ray transform)

24
Q

Reconstruction of backprojection?

A

acquisition : we know the line where the detected photons came from

“Reconstruction”: photon could have originated anywhere along the back-projected line; assign counts along line with equal probability, proportional to detected counts (back projection)

25
Q

How do we solve the fact that back projection gives us a very smooth version of the original

A

we will need to apply a sharpening filter.

This can be done before or after backprojection.

Before: Filtered back projection (FBP)

After: Back project and filter (BPF)

26
Q

FBP issues?

A

Need to discretise analytic formulas - how do i discretise fourier transforms??

Analytic methods ignore various effects

  • Noise (has to be handled by filtering)
  • Finite detector size
  • Limited number of angles - in surgery you cannot

(you can try and use different maths to solve some of these problems but not all of them)

27
Q

What is the fundamental trade - off that we have in medical imaging all of the time?

A

contrast vs noise

28
Q

Noise is all-important in emission tomography. It is determined by

A
  • the amount of detected counts
  • the choice of image reconstruction algorithm
29
Q

KEY POINT : FBP pros and cons?

A

It is fast

but

inflexible and can lead to noisy images

30
Q
A