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The compact compander is a measurable finite quantizer

Statement

For the data in Positive C1 compact one-dimensional compander, every cell is Borel, the cells partition [a,b], the index map is measurable, and DN(f,g) is finite for each N≥1.

Facts & Assumptions

Given: a<b, positive normalized C1 densities f,g on [a,b], and an integer N≥1.

[F1]

Positive C1 compact one-dimensional compander: βj=ϕ(j/N) are the cell boundaries, rj=ϕ((j−12)/N) are the reproduction points, and the cells are half-open except for the final cell containing b.

[F2]

A positive C1 point density has a C2 cumulative inverse: ϕ is a strictly increasing bijection from [0,1] to [a,b].

[F3]

Finite measurable squared-error quantizer and nearest-center rule: a finite quantizer is a Borel map into a finite discrete index set and its distortion is the integral of squared reconstruction error.

Proof

1.1givenF1F2

The boundary sequence β0<⋯<βN is strictly increasing by [F2], with β0=a and βN=b. Thus the intervals in [F1] are pairwise disjoint Borel sets whose union is [a,b].

2.1givenF1F2F3step 1.1algebra∎

Each index preimage is one of those Borel intervals, so the finite-valued index map is Borel and defines a quantizer as in [F3]. Each reproduction point lies in [a,b] by [F1] and [F2], so ∣x−rj∣≤b−a on cell j; hence 0≤DN(f,g)≤(b−a)2∫abf(x) dx=(b−a)2<∞.

Depends on

Used by

Cited to discharge well-definedness by Positive C1 compact one-dimensional compander.

Dependency tree · two levels

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