Published by Patrick Mutisya · 14 days ago
X-rays are produced when high‑energy electrons are decelerated or when they strike a high‑Z target material. Two main mechanisms are:
The X‑ray tube consists of a cathode that emits electrons via thermionic emission, an accelerating anode (usually tungsten), and a vacuum chamber. The accelerating voltage is typically 30–150 k \cdot for diagnostic imaging.
X-ray photons have energies ranging from a few ke \cdot to several hundred keV. Their penetration ability depends on energy and material density. Typical applications include:
| X-ray Type | Energy Range (keV) | Typical Application |
|---|---|---|
| Low‑energy (30–70) | 30–70 | Dental imaging, mammography |
| Medium‑energy (70–120) | 70–120 | Standard radiography, CT scans |
| High‑energy (120–300) | 120–300 | Bone densitometry, industrial inspection |
Radiation safety follows the ALARA principle (As Low As Reasonably Achievable). Key measures include:
In positron emission tomography (PET), a radiotracer containing a positron‑emitting isotope (e.g. \$^{18}\$F) is injected into the body. The positron (\$e^+\$) travels a short distance before encountering an electron (\$e^-\$) and annihilating:
\$e^+ + e^- \;\rightarrow\; \gamma + \gamma\$
Each gamma photon carries an energy of \$511 \text{ keV}\$ (half the rest mass energy of the electron/positron pair). The two photons are emitted approximately 180° apart.
Detectors surrounding the patient convert gamma photons into electrical signals. Common detector technologies include:
Coincidence detection requires that two detectors record photons within a narrow time window (typically \$10\,\text{ns}\$). This establishes a line of response (LOR) along which the annihilation event occurred.
Time‑of‑flight (TOF) PET adds the difference in arrival times of the two photons to localise the event along the LOR. The position \$x\$ along the LOR is given by:
\$x = \frac{c\,\Delta t}{2}\$
where \$c\$ is the speed of light and \$\Delta t\$ is the measured time difference. Processing the arrival times for many events allows reconstruction of the tracer concentration distribution using algorithms such as filtered back‑projection or iterative maximum‑likelihood expectation‑maximisation.
Key advantages of PET include high sensitivity, quantitative capability, and the ability to combine with CT or MRI for anatomical localisation.