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TauCeti.Analysis.CompletelyMonotone.Stieltjes.Inversion

Inversion of the parameter of Stieltjes and complete Bernstein functions #

The substitution t ↦ t⁻¹ exchanges the two ends of (0, ∞), and the Stieltjes class is stable under the normalized substitution f ↦ (t ↦ f(t⁻¹) / t). On representing data it acts by exchanging the singular coefficient a of a / t with the constant coefficient b, and by the measure transformation

μ ↦ ν, the image of x⁻¹ μ(dx) under x ↦ x⁻¹,

because for x > 0 the kernels satisfy (t⁻¹ + x)⁻¹ / t = x⁻¹ (t + x⁻¹)⁻¹. This measure transformation, MeasureTheory.Measure.stieltjesInversion, preserves the Stieltjes weight condition, never charges 0, and is an involution on measures without an atom at 0. Consequently the substitution is an involution of the Stieltjes class modulo equality on (0, ∞).

Combined with the correspondence f ↦ t f(t) between Stieltjes and complete Bernstein functions, this yields two further standard dualities: f is Stieltjes exactly when t ↦ f(t⁻¹) on (0, ∞) extends to a complete Bernstein function, and for a complete Bernstein function f, the function t ↦ t f(t⁻¹) on (0, ∞) extends to a complete Bernstein function.

Main declarations #

References #

The measure transformation dual to the substitution t ↦ t⁻¹ in a Stieltjes representation: the image of the measure x⁻¹ μ(dx) under x ↦ x⁻¹. The density x⁻¹ is taken in ℝ≥0, so it vanishes at x = 0 and the transformed measure never charges 0.

Equations
Instances For

    Integration against stieltjesInversion μ in terms of μ.

    Lower Lebesgue integration against stieltjesInversion μ in terms of μ.

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    Integrability against stieltjesInversion μ in terms of μ.

    @[simp]

    The transformed measure never charges 0, because its density vanishes there.

    stieltjesInversion is an involution on measures without an atom at 0.

    The transformed measure satisfies the Stieltjes weight condition exactly when the restriction of the original measure to (0, ∞) does. Indeed x⁻¹ (1 + x⁻¹)⁻¹ = (1 + x)⁻¹ for x > 0.

    The transformed measure satisfies the Stieltjes weight condition exactly when the original measure does, provided the latter has no atom at 0.

    Inversion of a Stieltjes representation. If (μ, a, b) represents f, then t ↦ f(t⁻¹) / t is represented by (stieltjesInversion μ, b, a): the singular and constant coefficients are exchanged.

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    The substitution f ↦ (t ↦ f(t⁻¹) / t) is reversible on representing data: (ν, b, a) represents t ↦ f(t⁻¹) / t exactly when (stieltjesInversion ν, a, b) represents f, for any ν without an atom at 0.

    If f is a Stieltjes function, then so is t ↦ f(t⁻¹) / t.

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    The Stieltjes class is invariant under the involution f ↦ (t ↦ f(t⁻¹) / t).

    Stieltjes functions and complete Bernstein functions under inversion. A function f is Stieltjes exactly when t ↦ f(t⁻¹) on (0, ∞) extends to a complete Bernstein function on [0, ∞).

    Duality of complete Bernstein functions. If f is a complete Bernstein function, then t ↦ t f(t⁻¹) on (0, ∞) extends to a complete Bernstein function on [0, ∞).