Feynman Path Integral

K(b,a) = ∫ D[x(t)] exp(iS[x]/ℏ) — every path contributes, classical path dominates

Physics

Propagator = sum over all paths
K(x_f,t_f;x_i,t_i) = ∫D[x] e^{iS/ℏ}

S[x] = ∫L dt = ∫(½mẋ²−V) dt

Classical path: δS = 0 (stationary)
ℏ→0: only classical path survives
Quantum: all paths interfere

Parameters

Path Statistics

Paths shown
Classical action S_cl
|K|² (prob. density)
Color = phase e^{iS/ℏ}
Bright = near stationary phase
(near-classical paths)
Sum ≈ amplitude at endpoint

Controls

Stationary phase approximation:
Non-classical paths cancel
via rapid oscillation
Classical path contributes most