Equations (16)-(17): the two source branches in their original distance variables #
Equation (17), second distance moment.
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Equation (17), endpoint value of the auxiliary potential.
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theorem
Papers.AnsariRockelSteinmassl2026RhoGamma.right_source_data
(S : ProbabilityTheory.Copula.RankRegion.RhoFootrule.RightData)
:
have ell := 1 / (2 * (↑S.N + 1));
ProbabilityTheory.Copula.RankRegion.RhoFootrule.UpperSpline.period (↑S.N) S.v S.w = 2 * ell + S.v ∧ ∫ (x : Fin 2 → ↑unitInterval), |↑(x 0) - ↑(x 1)| ∂S.copula.toMeasure = sourceMean S.N ell S.v ∧ ∫ (x : Fin 2 → ↑unitInterval), (↑(x 0) - ↑(x 1)) ^ 2 ∂S.copula.toMeasure = sourceSquare S.N ell S.v ∧ ProbabilityTheory.Copula.RankRegion.RhoFootrule.UpperSpline.offset (↑S.N) S.v S.w = sourceOffset S.N ell S.v
On the right branch, the source delta is the library's nonnegative v.
theorem
Papers.AnsariRockelSteinmassl2026RhoGamma.left_source_data
(S : ProbabilityTheory.Copula.RankRegion.RhoFootrule.LeftData)
:
have ell := 1 / (2 * ↑S.N);
ProbabilityTheory.Copula.RankRegion.RhoFootrule.UpperSpline.period (↑S.N) S.v S.w = 2 * ell - S.v ∧ ∫ (x : Fin 2 → ↑unitInterval), |↑(x 0) - ↑(x 1)| ∂S.copula.toMeasure = sourceMean S.N ell (-S.v) ∧ ∫ (x : Fin 2 → ↑unitInterval), (↑(x 0) - ↑(x 1)) ^ 2 ∂S.copula.toMeasure = sourceSquare S.N ell (-S.v) ∧ ProbabilityTheory.Copula.RankRegion.RhoFootrule.UpperSpline.offset (↑S.N) S.v S.w + S.v * S.w = sourceOffset S.N ell (-S.v)
On the left branch, the source delta is minus the library's v.
noncomputable def
Papers.AnsariRockelSteinmassl2026RhoGamma.sourceRight
(N : ℕ)
(hN : 0 < N)
(s : ℝ)
(hlo : 1 / (↑N + 1) ≤ s)
(hhi : s ≤ 1 / (2 * ↑N) + 1 / (2 * (↑N + 1)))
:
Construct the source's right branch at its auxiliary multiplier s.
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- One or more equations did not get rendered due to their size.
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noncomputable def
Papers.AnsariRockelSteinmassl2026RhoGamma.sourceLeft
(N : ℕ)
(hN : 0 < N)
(s : ℝ)
(hlo : 1 / (2 * ↑N) + 1 / (2 * (↑N + 1)) ≤ s)
(hhi : s ≤ 1 / ↑N)
:
Construct the source's left branch at its auxiliary multiplier s.
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- One or more equations did not get rendered due to their size.