Vertex detector
The innermost layer of silicon pixels sits only a few centimetres from the collision point. It measures tracks to a few micrometres and finds where they originate. Particles such as B hadrons or the tau fly from a fraction of a millimetre up to several millimetres before they decay – a displaced secondary vertex gives them away.
Boosts particles with displaced decays: τ, J/ψ, B hadrons, top, LQ and N.
Boosts
Tracker
Silicon strips and pixels measure the flight path of charged particles at many points. A magnetic field (CMS 3.8 T, ATLAS 2 T) bends the paths: the radius gives the momentum, p ≈ 0.3 · B · r (p in GeV/c, B in tesla, r in metres), the direction of the bend gives the sign of the charge. Neutral particles leave no track.
Boosts charged particles that leave tracks: π, K, p, W and heavy charged particles.
Boosts
Calorimeter
Electrons and photons start a shower of electrons, positrons and photons in dense material until all the energy is absorbed and measured (ATLAS: lead and liquid argon, CMS: lead-tungstate crystals). The Higgs boson, too, was found in 2012 through decays into two photons.
Boosts the electron, photon, Higgs and other particles that deposit their energy here.
Boosts
Muon chambers
Muons are about 200 times heavier than electrons, radiate little and therefore penetrate everything in front of them. That is why the drift tubes and chambers sit on the outside: whatever still gives a signal there is almost always a muon. Decays like Z → μμ are thus especially clean to spot.
Boosts the muon, Z, Z′ and A′. Higher levels add outer stations – the detector grows.
Boosts