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TauCeti.Analysis.PositiveDefinite.SemigroupGroup.FourierLaplace.ZeroSpatial

The zero-spatial Berg--Christensen--Ressel theorem #

When the spatial inner-product space in the Berg--Christensen--Ressel representation is the zero space PUnit, its Laplace--Fourier transform has no Fourier factor and is just a Laplace transform. This file makes that specialization precise at both the measure and theorem levels.

The measurable equivalence ℝ≥0 × PUnit ≃ᵐ ℝ≥0 identifies finite representing measures. Under this equivalence, TauCeti.RepresentsLaplaceFourier for the function (t, _) ↦ f t is exactly TauCeti.RepresentsLaplace for f. Consequently the bounded, continuous positive-definite condition in the BCR theorem is equivalent to complete monotonicity on the closed half-line. Thus the zero-spatial case of BCR is precisely the Hausdorff--Bernstein--Widder theorem, including uniqueness of the representing measure.

Main declarations #

References #

@[simp]

The Laplace--Fourier transform of a measure transported to ℝ≥0 × PUnit is its ordinary Laplace transform, viewed in ℂ.

In zero spatial dimension, Laplace--Fourier representation of (t, _) ↦ f t by the transported measure is exactly ordinary Laplace representation of f.

@[simp]

A measure on ℝ≥0 × PUnit represents a zero-spatial function if and only if its time marginal gives the corresponding Laplace representation.

The zero-spatial BCR theorem is the Hausdorff--Bernstein--Widder theorem.

For a real function f, the bounded, continuous positive-definite condition on (t, _) ↦ f t : ℝ≥0 × PUnit → ℂ holds exactly when f is continuous on [0, ∞) and completely monotone on (0, ∞).

In zero spatial dimension, the transported Bernstein measure represents a function that is continuous on [0, ∞) and completely monotone on (0, ∞).

Any zero-spatial BCR representing measure is the transported Bernstein measure.