NUKS Flashcards
Beta minus
too many?
what’s emitted?
What kind of transition
Too many neutrons
N > P
electron (beta particle) emitted from nucleus
Neutrino also emitted to balance energy
ISOBARIC - neutron and proton have same mass
ATOMIC NUMBER GOES UP
Beta emitter shielding?
PLASTIC
low Z
High Z would produce Brems
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Beta Minus
Energy down, Z up
I
I
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Energy lost and Z goes down
Proton to neutron
Beta positive decay
requires 1.02 MeV
Positron and a neutrino
511 keV x2 when positron hits electron
ISOBARIC
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No steep initial drop
loss of proton and energy
ELECTRON CAPTURE
ISOBARIC
isobaric transitions
Beta emission
positron emission
electron capture
“Isometric transitions”
when do they occur?
after an isobaric (A the same) transition
leftover energy released
Gamma emission
what type of transition
isomeric transition
nucleus emits extra energy
I
I
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Between Isobaric transition and subsequent isomeric (GAMMA EMITTING) transitions
These usually happen bam bam, but some hang out for a minute before gamma emission, these are METASTABLE
Tc 99m example of isobaric metastable isomeric
Mo99 —> Tc99m (ISOBARIC Beta MINUS, electron emitted)
Tc99m ——> Tc99 (ISOMERIC, gamma photon (140keV))
Tc99m hangs out as metastable for a couple hours
Enemy of gamma photon emission
Internal conversion
instead of gamma emission
energy given to an electron —–> characteristic Xray or Auger
Alpha decay
use?
helium nuclei
2 protons, 2 neutrons
Slow and fat
rare treatmentn situations
bone pain cancer mets via rAdium 223 (Alpha2protons2 neutrons)
Production
Bombardment
Striking targets with
Neutrons - in a reactor
Charged particles (alpha, protons, deuterons) - in a cyclotron
Bombardment
downside to using a reactor
(bombarding with neutrons)
Leftover parent to clean up
NOT “carrier free”
Cyclotron produces via transmutation, no parents to clean up, “carrier free”
Production
Fission
Neutrons fired into large elements
split into pieces, random crap made
effective half life formula
1/effective = 1/physical + 1/biologic
What does ‘activity’ measure
units
Specific activity
disintegrations per second
Curie = Ci = 3.7x10^10 disintegrations per second
SI unit = becquerel Bq = one disintegration per second
Specific activity = activity per unit mass (Bq/g)
(longer half life = lower specific activity)
Gamma camera general set up
Photons
Collimator
Crystal
PMT’s
computer
gamma photons –> light pulse –>voltage –> picture
MC collimator “work horse”
parallel hole
Parallel hole energies and examples
low
medium
high
LOW 1 - 200 keV (Tc99, I123, Xe133, TI201)
MEDIUM 200-400 keV (Ga67, In111) (medium needs to GaIn)
High > 400 keV (I131)
Sensitivity and Resolution
when are high sensitivity collimators good
Inversely related
High sensitivity collimator allows twice as many counts to be imaged with shitty resolution
High sensitivity good for dynamic imaging (flow phase)
Distance effect on sensitivity and resolution
NO EFFECT on sensitivity (net counts the same, bigger FoV)
Resolution WORSENS with distance
Pinhole collimator
what does?
what for?
?mag
magnifies and inverts
thyroids and small parts
pinhole to detector = f
patient to pinhole = b
F>B = mag
Pinhole cons
distorts large objects
Shitty sensitivity