t = 0
⟨x⟩ = —
σ_x = —
⟨x⟩ = —
σ_x = —
Split-operator: e^{-iHΔt} ≈ e^{-iV Δt/2} · e^{-iT Δt} · e^{-iV Δt/2}. The kinetic part is diagonal in momentum space (FFT → multiply → IFFT).
Free spreading: σ(t)² = σ₀² + (t/2mσ₀)² — quantum dispersion has no classical analogue.
Free spreading: σ(t)² = σ₀² + (t/2mσ₀)² — quantum dispersion has no classical analogue.