No state turns orthogonal before πħ / (2ΔE)
The survival amplitude A(t) = ∑ pk e−iEkt
is the sum of the arrows on the right. Mandelstam–Tamm, proved in Lean:
‖A(t)‖ ≥ cos(ΔE·t) until ΔE·t = π/2. The arrow tip can never enter the
orange disc; the disc shrinks to nothing exactly at π/2.
‖A(t)‖ against ΔE·t / ħ
‖A(t)‖
floor cos(ΔE·t), Lean
forbidden
Phasors pk e−iEkt, tip to tail
ΔE·t / ħ
–
‖A(t)‖
–
floor cos(ΔE·t)
–
margin
–
Two equal branches touch the floor at every time and reach zero exactly at π/2:
the constant cannot be improved. Every other spectrum stays strictly above. Energies are
rescaled so that ΔE = 1 and centred so that ⟨E⟩ = 0 (a global phase). Lean:
MandelstamTamm1945.cos_le_norm_amplitude, orthogonality_time,
and on ℂ^d, cos_le_norm_inner_evolve —
source.