Nuclear Med Flashcards
SPECT - Compared to Gamma Camera
Better contrast
Worse spatial resolution than gamma
Higher noise than gamma
PET - Compared to SPECT
Better spatial resolution
Less noise
SPECT has better contrast
Decay Patterns
M -4 ALPHA DECAY (too many protons or neutrons)
A -2
M 0 BETA -VE DECAY (too many neutrons). Neutron converted to proton in nucleus and an electron and antineutrino released from the nucleus)
A +1
M 0 BETA +VE DECAY (too few neutrons) (positron produced)
A -1
M 0 ELECTRON CAPTURE (too few neutrons). A proton captures an electron from one of the shells
A -1 (starts with K) and converts to neutron. Iodine 123 decays this way producting a gamma wray and x-ray (given off as a result of hole in electron shell)
M 0 ISOMERIC TRANSITION (decay of radionuclide to ground state giving off gamma radiation as in Tn-99m)
A 0
Positrons
Same mass as electrons (1/1840)
Only exist while they have energy
Positive charge
PET
30,000 bismuth detectors
Gamma photons 511keV produced by annihilation between electron and positron
Fluorine decays by beta positive decay
The activity from each point source can be measured as a sine curve or sonogram
Spatial resolution 4-5mm
PET Detectors
Good energy resolution
High detection efficiency
Short scintillation decay time
High atomic number and physical density
High light output
SPECT
Camera moves in 3 or 6 degree increments
- can be continuous or step and shoot
Produces 3D images
Spatial resolution 15-20mm
Contrast good in SPECT
Cyclotron
Cyclotron
67Gallium
111Indium
123Iodine
201Tl
Gamma Camera
Gamma Camera
- 100 photomultiplier tubes that determine position and intensity of photons
- Technetium is a pure GAMMA EMITTER
- Lead collimator thickness varies:
- 0.3mm
- 1mm
- 2mm
Typical sensitivity is up to 2%
(Around 75-90% of gamma photons are detected)
Scattered photons can still be accepted if energy is within the photopeak
Photomultiplier tube contains a series of dynodes
Gamma Camera
Gamma Camera
-spatial resolution is made better by either
—making collimator holes smaller
—making lead septa thicker
—making collimator thicker
This however will reduce the number of gamma photons reaching the scintillation crystal (will hit collimator instead) and therefore sensitivity will decrease
Photomultipliers and count rate do NOT affect spatial resolution
Metal objects can cause artefact in Gamma cameras bu absorbing some of the gamma rays which result in appearance of a possible ‘cold lesion’
Photopeak
- Photopeak is produced by pulses that are a result of photoelectric interaction
- ‘Pulse pile up’ is caused by two or more photons being detected at same time. This peak occurs to the right of the main photopeak
Photomultiplier
Needs a photocathode for operation (converts light into electrons)
- Photocathode releases 1 electron for every 5-10 photons
- Photomultipler contains a series of dynodes than amplify electrons
- 10-12 dynodes, each more positive in potential than the last
- each dynode has potential difference of 1.2kV (total potential 1-1.2kV
- each dynode releases 4 electrons for every electron that hits it
Pulse Height Analyser
Reduces noise!!
Located between detector and counting system
Can detect more than one photo-peak
Wide window produces images faster but they are of lower quality due to scatter and lower energy photons
Narrow window produces better quality image
Collimator allows location of the source of gamma photons within patient (primary purpose is not to filter out scattered radiation. Pulse height analyser does this)
The use of collimators improves spatial resolution
Quality Control in Gamma
Field Uniformity (Test of detector)
-Field uniformity refers to the ability to produce a uniform distribution of activity
Can be tested using a flat, sealed plate of cobalt 57 called a flood field or sheet phantom
- Intrinsic floods performed WITHOUT collimator (addition of a collimator reduces intrinsic resolution)
- Extrinsic floods performed WITH collimator
Modern cameras have uniformity of at least 2%
Quality Control in Gamma
Spatial Resolution
Tested using a Line Source which results in creation of a graph called the Line Spread Function
- From this we can measure FWHM which is used to compare resolutions of different systems
- Gamma camera resolution generally 5-10mm
- Intrinsic resolution 3-4mm (intrinsic resolution is always the best)
- FWHM is a measure of spatial resolution of a system
Collimators in Gamma Camera
Collimator allows location of the source of gamma photons within patient (primary purpose is not to filter out scattered radiation. Pulse height analyser does this)
The use of collimators improves spatial resolution
There is a trade off between collimator sensitivity and spatial resolution
Increasing number of holes increases sensitivity!!
Increasing collimator sensitivity reduces patient dose (more gama rays passing through collimator measn less radionuclide needed hence lower patient dose. This results in lower spatial resolution however
Internal conversion
Gamma ray interacts with inner shell electrons via photoelectric effect releasing
Photoelectrons
Characteristic x rays
Examples: Iodine 125 and 123
Beta Particles
Beta Particles
- Are made up of electrons
- Negative electrons are negative beta particles
- Positive electrons are positrons
Beta particles follow a random path in matter like secondary electrons
Release as a continuous spectrum of energies (like bremmst)
NOT specific energies
Can only travel a few mm in tissue
Result in a trail of ionized atoms
Ideal Radiopharmaceutical Properties
Pure gamma emitter between 50 - 300keV
Half life suitable for examination
Half Lives
Krypton - 13 seconds
Fluorine - 110mins
Technetium 99 - 6 hours
Molybdenum 99 - 67 hours
Biological half life is dependent on the rate if ELIMINATION of the radionuclide from the body (NOT rate of radioactive decay)
The dose received by the organ is PROPORTIONAL to the effective dose
The pharmaceutical used does NOT affect the half life