Particle detection technology uses fast, sensitive detectors to capture subatomic events with high temporal resolution.Particle detection technology encompasses the instruments and methods used to observe and measure subatomic particles, from electrons and photons to exotic particles like muons. Modern detectors are designed to capture the position, energy, and arrival time of particles with extreme precision, often at rates of millions of events per second. This technology is the foundation of experimental particle physics, astrophysics, and medical imaging, enabling discoveries from the Higgs boson to the mapping of the human brain's activity.
The field began with the cloud chamber, invented by Charles Wilson in 1911, and evolved through spark chambers, bubble chambers, and silicon detectors. The development of the photomultiplier tube in the 1930s was a key step for fast timing.
Most particle detectors rely on converting the energy of a passing particle into a measurable signal. In semiconductor detectors, a charged particle creates electron-hole pairs that are swept away by an electric field, producing a current pulse. In scintillators, the particle excites atoms that emit light, which is then captured by photodetectors. Time-of-flight systems measure the time it takes a particle to travel between two points, giving its velocity. To achieve high temporal resolution, detectors use fast electronics and materials with short response times, allowing the precise timing of events that occur in quick succession.
Particle detectors are used in medical imaging (PET scanners), radiation monitoring, and high-energy physics experiments like those at the Large Hadron Collider.
Modern particle detectors can timestamp events with an accuracy of tens of picoseconds, allowing them to distinguish particles traveling at nearly the speed of light that are separated by just a few millimeters.
| P | variable | Detection probability of a particle — probability |
| M | variable | Mass of the particle — mass kilogram |
| a | variable | Proper acceleration of the detector — acceleration metre per second squared |
| c | constant | Speed of light in vacuum — speed of light = 299792458 metre per second |
| ħ | constant | Reduced Planck constant — reduced planck constant = 1.054571817e-34 joule second |
| P(r) | variable | capture probability at radius r — probability |
| r | variable | radial coordinate — radius metre |
| r_c | variable | outer horizon radius — radius metre |
| r_H | variable | inner horizon radius — radius metre |
| u | variable | integration variable — radius metre |
| f(u) | variable | metric function — metric function |
| ∫ | operator | computes the area under the curve of the integrand — integral operator |
| √ | operator | computes the principal square root — square root |











