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Papers.Rockel2026XiFootrule.TwoParameter

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The two-parameter family in Section 3.2 #

The displayed density is identified with an actual copula law. The proof uses probability-integral transforms and almost-everywhere quantile inversion, so zero marginal densities and the closed-square parameter endpoints are covered.

noncomputable def Papers.Rockel2026XiFootrule.twoParameter (α β : ℝ) (hα : α ∈ Set.Icc 0 (1 / 2)) (hβ : β ∈ Set.Icc 0 (1 / 2)) :
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    The pre-standardization law has the claimed two marginal distributions.

    theorem Papers.Rockel2026XiFootrule.twoParameter_marginal_density (α β : ℝ) (hα : α ∈ Set.Icc 0 (1 / 2)) (hβ : β ∈ Set.Icc 0 (1 / 2)) (t : ↑unitInterval) :
    have B := Verification.diagonalHoleBand α β hα hβ; B.columnDensity t = (1 - B.holeLength t) / (1 - β)

    Equation (31) evaluates the actual second marginal, rather than a candidate normalization.

    theorem Papers.Rockel2026XiFootrule.twoParameter_density (α β : ℝ) (hα : α ∈ Set.Icc 0 (1 / 2)) (hβ : β ∈ Set.Icc 0 (1 / 2)) :

    Proposition 3.5 and Equation (32), including both parameter endpoints.

    A zero-width hole gives independence along the entire bottom parameter edge.

    The upper corner is the same actual checkerboard as in Theorem 3.4.

    theorem Papers.Rockel2026XiFootrule.twoParameter_corner_coefficients :
    (twoParameter (1 / 2) (1 / 2) ⋯ ⋯).chatterjeeXi = 1 / 2 ∧ (twoParameter (1 / 2) (1 / 2) ⋯ ⋯).spearmanFootrule = -1 / 2

    The corner's exact rank values; no numerical evaluation.

    Equation (33) stays inside the proved closed parameter square for every finite mu.