Hausdorff--Bernstein--Widder theorem #
This file proves the finite-measure form of the Hausdorff--Bernstein--Widder theorem for
completely monotone functions on the closed half-line: a function is continuous on [0, ∞)
and completely monotone on (0, ∞) if and only if it is the Laplace transform of a (unique)
finite positive measure on ℝ≥0.
The hard direction is a direct application of the finite-difference representation theorem in
FiniteDifference/Laplace.lean: derivative complete monotonicity implies the mixed-difference
condition, and continuity on [0, ∞) supplies right-continuity at zero. The easy direction and
uniqueness live in Laplace/Representation.lean.
Main declarations #
TauCeti.exists_representsLaplace_of_isContinuousCompletelyMonotoneOnIoiTauCeti.hausdorff_bernstein_widder,TauCeti.hausdorff_bernstein_widder_existsUniqueTauCeti.bernsteinMeasure: the canonical representing measure, with its uniqueness, total-mass, and algebraic API.
References #
The finite-measure representation is the Hausdorff--Bernstein--Widder theorem, after S. Bernstein (1928) and D. V. Widder, The Laplace Transform, Chapter IV.
- Roadmap:
TauCetiRoadmap/OneParameterSemigroups/README.md, Part B (Bernstein theorem milestone).
Existence half of the Hausdorff--Bernstein--Widder theorem: a function continuous on
[0, ∞) and completely monotone on (0, ∞) is the Laplace transform of a finite positive
measure on ℝ≥0.
Headline theorem #
Hausdorff--Bernstein--Widder theorem, finite-measure version on ℝ≥0.
A function is continuous on [0, ∞) and completely monotone on (0, ∞) if and only if it is
the Laplace transform of a finite positive measure on ℝ≥0.
Unique-existence form of the Hausdorff--Bernstein--Widder theorem.
The canonical representing measure #
The Bernstein representing measure of f: the unique finite measure on ℝ≥0 whose
Laplace transform is f on [0, ∞), when f has one, and the zero measure otherwise.
By TauCeti.hausdorff_bernstein_widder a representing measure exists exactly when f is
continuous on [0, ∞) and completely monotone on (0, ∞).
Equations
- TauCeti.bernsteinMeasure f = if h : ∃ (μ : MeasureTheory.Measure NNReal), TauCeti.RepresentsLaplace μ f then h.choose else 0
Instances For
Outside the hypotheses of the Hausdorff--Bernstein--Widder theorem the Bernstein measure is
0.
The Bernstein measure represents its function.
The Bernstein measure of any function is finite: for a represented function this is the
finiteness of its representing measure, and otherwise the measure is 0.
Uniqueness of the Bernstein measure. Any finite measure representing f by its Laplace
transform is the Bernstein measure of f. No hypothesis on f is needed: a represented function
is automatically continuous and completely monotone.
The Laplace transform of the Bernstein measure recovers the function on [0, ∞).
The total mass of the Bernstein measure is the value of the function at 0.
The total mass of the Bernstein measure, as an extended nonnegative real.
A function with total mass 1 has a probability measure for its Bernstein measure.
The Bernstein measure of the zero function is the zero measure.
The Bernstein measure turns sums of functions into sums of measures.
The Bernstein measure turns nonnegative scalar multiples of functions into scalar multiples of measures.