detector-physics

Layer 1 — Physics24 concepts in this subtree

Instrumentation physics of particle and radiation detectors. Principles: ionisation (Bethe-Bloch), Cherenkov radiation threshold β>1/n, transition radiation X→Y at media interfaces, scintillation light yield in organic (stilbene,…

Calorimeter energy resolution: σ(E)/E = a/√E ⊕ b/E ⊕ c (stochastic ⊕ noise ⊕ constant)
Cherenkov radiation: threshold β > 1/n, opening angle cos θ_C = 1/(β·n)
Time-of-flight particle ID: Δt = (L/c)·(√(1+m₁²/p²) − √(1+m₂²/p²)) ≈ L m₁²/(2p²c) for m≪p
Silicon microstrip spatial resolution: σ = p/√12 (binary), p/(S/N) charge-division
Scintillator light yield: ~40 γ/keV NaI(Tl), ~10 γ/keV BGO, ~9 γ/keV plastic
Transition radiation (Ginzburg-Frank): ⟨E⟩ ∝ γ · ω_p·(Z_p·ω)/(3c); Lorentz-factor ID
Bethe-Bloch: -dE/dx = K·z²·(Z/A)·(1/β²)·[½·ln(2m_ec²β²γ²T_max/I²) - β²]
Ramo-Shockley: i(t) = -q·v·∇ψ_w(x); weighting potential as Laplace Green's
Landau straggling: energy-loss MPV Δ=ξ·[log(2m_ec²β²γ²ξ/I²)+0.200-β²]
Bethe-Bloch: z²-scaling ratio z=2/z=1 = 4; Legendre ⟨P2,P2⟩=2/5; ⟨P1,P2⟩=0
Ramo: i=-q·v/d_gap; Q_induced=-q; Δψ_w=0; ψ_w(0)=0, ψ_w(d)=1
Landau MPV Δ=ξ·[log(2m_ec²β²γ²ξ/I²)+1/5-β²]; FT gauss = √π exp(-π²k²/a)/√a
Super-Kamiokande neutrino observatory
PMT (Iams-Salzberg 1936)
SiPM (Buzhan 2003)
Calorimetry
Cherenkov radiation (1934-1937)
CMOS pixel (DEPFET)
Geiger counter (1908)
Cloud chamber (Wilson 1911)
MWPC (Charpak 1968)
Cherenkov (1934)
Silicon strip (Heijne 1980)
Calorimeter (Fabjan-Gianotti 2017)
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