PET imaging: timing a positron tracer
Compare the decay curves of ¹⁸F, ¹¹C, ⁶⁸Ga and ¹⁵O, see why hospitals pair a cyclotron with a radiochemistry lab, and follow the positron annihilation that lights up the scan.
Goal
Match each tracer's half-life to its logistics, apply to plan a scan, and explain the → signal.
Apparatus and reagents
Virtual bench: decay curves of four positron emitters plus the annihilation scheme (511 keV each).
Procedure
- Select ¹⁸F-FDG. Check the curve at 110 min, 220 min and 330 min: what fractions remain?
- Switch to ¹⁵O (T½ = 2 min). How much activity is left after 8 minutes? Why can it only be made on-site?
- Compare ¹¹C and ⁶⁸Ga: which one survives a 90-minute synthesis, and which fits a 20-minute chemistry?
- Use the compare preset to rank the three isotopes by decay speed, then connect each to cyclotron, generator or regional distribution.
What to observe
- After one half-life exactly half remains, after three only an eighth — the grey 0.5 line and red tick always intersect the curve at T½.
- ¹⁵O loses 15/16 of its activity in 8 minutes while ¹⁸F keeps about 95% — half-life dictates how far a tracer can travel.
- The detected signal is not the positron itself but the two back-to-back 511 keV γ-rays from its annihilation with an electron.
Explanation
A proton-rich nucleus like decays by emission: . The positron flies a millimetre or so, meets an electron and annihilates into two 511 keV photons emitted back-to-back; a ring of detectors catching both at once draws a line through the annihilation point, and millions of lines rebuild the tracer map. Activity follows , so the half-life sets the whole logistics: ¹⁵O demands an on-site cyclotron, ¹¹C fits fast chemistry, ⁶⁸Ga is milked from a ⁶⁸Ge generator, and ¹⁸F (110 min) can be shipped to regional hospitals.
History of the experiment
Chemists behind it
Virtual experiment: a simplified model to build intuition. It does not replace real lab work or safety training; never repeat chemistry at home without supervision.