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Papers.Rockel2026ExactBlest.ExactBlestRho

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The complete rho/Blest region of exact-blest-regions.tex in natural parameters. Supporting inequalities use explicit potentials, independently of the general rearrangement lemma. Boundary-copula uniqueness is not asserted.

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      theorem Papers.Rockel2026ExactBlest.rho_param_cell00 (t x z : ℝ) (hz : 0 ≤ z) :
      0 ≤ 4 / 3 * |x - t / 2| ^ 3 + (z ^ 3 / 12 - t ^ 2 * z / 4) - (x ^ 2 - t * x) * z
      theorem Papers.Rockel2026ExactBlest.rho_param_cell01 (t x z : ℝ) (ht : 0 ≤ t) (hx : x ∈ Set.Icc 0 t) (hz : t ≤ z) :
      0 ≤ 4 / 3 * |x - t / 2| ^ 3 + (z ^ 3 / 3 - t * z ^ 2 / 2) - (x ^ 2 - t * x) * z
      theorem Papers.Rockel2026ExactBlest.rho_param_cell10 (t x z : ℝ) (ht : 0 ≤ t) (hx : t ≤ x) (hz : z ∈ Set.Icc 0 t) :
      0 ≤ 2 * x ^ 3 / 3 - t * x ^ 2 / 2 + (z ^ 3 / 12 - t ^ 2 * z / 4) - (x ^ 2 - t * x) * z
      theorem Papers.Rockel2026ExactBlest.rho_param_cell11 (t x z : ℝ) (ht : 0 ≤ t) (hx : t ≤ x) (hz : t ≤ z) :
      0 ≤ 2 * x ^ 3 / 3 - t * x ^ 2 / 2 + (z ^ 3 / 3 - t * z ^ 2 / 2) - (x ^ 2 - t * x) * z
      theorem Papers.Rockel2026ExactBlest.rho_param_dual (t x z : ℝ) (ht : 0 ≤ t) (hx : 0 ≤ x) (hz : 0 ≤ z) :
      (x ^ 2 - t * x) * z ≤ rhoParamPhi t x + rhoParamPsi t z
      noncomputable def Papers.Rockel2026ExactBlest.rhoPhiLo (t x : ℝ) :
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        noncomputable def Papers.Rockel2026ExactBlest.rhoPhiMid (t x : ℝ) :
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          noncomputable def Papers.Rockel2026ExactBlest.rhoPhiHi (t x : ℝ) :
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            theorem Papers.Rockel2026ExactBlest.integral_rhoParamPhi (t : ↑unitInterval) :
            ∫ (u : ↑unitInterval), rhoParamPhi ↑t ↑u = ↑t ^ 4 / 24 - ↑t / 6 + 1 / 6
            theorem Papers.Rockel2026ExactBlest.integral_rhoParamPsi (t : ↑unitInterval) :
            ∫ (u : ↑unitInterval), rhoParamPsi ↑t ↑u = -↑t ^ 4 / 48 - ↑t / 6 + 1 / 12
            theorem Papers.Rockel2026ExactBlest.transport_rho_param_upper (C : ProbabilityTheory.Copula 2) (t : ↑unitInterval) :
            ∫ (x : Fin 2 → ↑unitInterval), (↑(x 0) ^ 2 - ↑t * ↑(x 0)) * ↑(x 1) ∂C.toMeasure ≤ ↑t ^ 4 / 48 - ↑t / 3 + 1 / 4
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              • One or more equations did not get rendered due to their size.
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                theorem Papers.Rockel2026ExactBlest.rpow_cube_four_thirds (x : ℝ) (hx : 0 ≤ x) :
                (x ^ 3) ^ (4 / 3) = x ^ 4

                The manuscript's Phi, with the agreeing branches joined at rho=0.

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                  The exact rho/nu set equality with the displayed 4/3-power boundary.