X‑rays are generated when high‑energy electrons are decelerated or when inner‑shell electrons are removed from atoms. The two principal mechanisms are:
The energy of an emitted photon is given by the Planck relation:
$$E = hu$$where $E$ is the photon energy, $h$ is Planck’s constant and $u$ is the frequency of the radiation.
Two major categories of application are:
PET scanning relies on the detection of two 511 ke \cdot photons produced when a positron emitted by a radioactive tracer annihilates with an electron. The tracer must undergo β⁺ decay:
$$\ce{_{Z}^{A}X -> _{Z-1}^{A}Y + e^{+} + u_e}$$The emitted positron travels a short distance in tissue, then annihilates with an electron, producing two photons travelling in (approximately) opposite directions. Coincidence detection of these photons allows reconstruction of the tracer distribution inside the body.
The most widely used PET tracer is fluorine‑18 labelled fluorodeoxyglucose (ⁱ⁸F‑FDG). It is a glucose analogue that participates in cellular metabolism, making it ideal for imaging metabolic activity.
| Tracer | Radioisotope | Half‑life | Decay mode | Typical use |
|---|---|---|---|---|
| ⁱ⁸F‑FDG | Fluorine‑18 | 110 min | β⁺ | Oncological imaging, brain metabolism |
| ⁸⁸Y‑DOTATATE | Yttrium‑88 | 106 min | β⁺ | Neuroendocrine tumour imaging |
| ¹¹C‑PiB | Carbon‑11 | 20 min | β⁺ | Alzheimer’s disease amyloid imaging |
All PET tracers share the essential feature of undergoing β⁺ decay, providing the positrons required for annihilation photon production.
Remember: