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temp_halves_on_double

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formal statement (Lean)

 180theorem temp_halves_on_double (bh₁ bh₂ : RSBH)
 181    (h : bh₂.mass = 2 * bh₁.mass) :
 182    rs_hawkingTemp bh₂ = rs_hawkingTemp bh₁ / 2 := by

proof body

Tactic-mode proof.

 183  unfold rs_hawkingTemp
 184  rw [h]
 185  have hM : bh₁.mass > 0 := bh₁.mass_pos
 186  have hpi : Real.pi > 0 := Real.pi_pos
 187  have hdenom : 8 * Real.pi * bh₁.mass ≠ 0 := by positivity
 188  field_simp [hdenom]
 189
 190/-! ## Theorem 4: Hamiltonian Approximation Bound -/
 191
 192/-- The Hamiltonian Ĥ emerges from the recognition operator R̂ only in the
 193    small-strain regime. For strain ε with |ε| ≤ 1/2:
 194
 195    J(1 + ε) = ε²/2 + c·ε³  where |c| ≤ 2
 196
 197    The ε²/2 term gives the quadratic Hamiltonian. The cubic correction
 198    is the R̂-specific term that standard physics misses. Near an
 199    ultramassive BH's accretion disk, ε is NOT small, so the Eddington
 200    limit (derived from the Hamiltonian approximation) underestimates
 201    the dynamics that R̂ permits. -/

depends on (13)

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