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Henstock–Kurzweil integrability on subintervals and additivity over adjacent intervals

Statement

Let a≤c≤b. A function is Henstock–Kurzweil integrable on [a,b] if and only if its restrictions to [a,c] and [c,b] are integrable, and then

∫abf=∫acf+∫cbf.

For compact HK integrals, define the oriented value by ∫vuf:=−∫uvf when u<v and ∫uuf:=0. With this convention, for points u,v,w, ∫uwf=∫uvf+∫vwf whenever the compact pieces are integrable.

For points u,v,w, ∫uwf=∫uvf+∫vwf whenever the compact pieces are integrable.

Henstock–Kurzweil integrals restrict to subintervals and add over adjacent intervals.

Facts & Assumptions

Given: A function on [a,b] and a cut point c∈[a,b].

[L1]

Every gauge on a compact interval admits a fine tagged partition (Cousin's lemma: every gauge on a compact interval admits a fine tagged partition).

[L2]

A function on a compact interval is Henstock–Kurzweil integrable if and only if, for every ε>0, there is a gauge such that every pair of fine tagged sums differs by less than ε (The Cauchy criterion for Henstock–Kurzweil integrability).

Proof

technique · direct
1.1givenL1L2algebra

For the forward direction, fix a whole-interval gauge whose fine sums are within ε/2 of the integral. Given two fine partitions P,Q of [a,c], use [L1] to choose one fine partition R of [c,b] for the restricted gauge. Then P∪R and Q∪R are whole-interval fine partitions, so ∣S(f,P)−S(f,Q)∣<ε; [L2] proves integrability on [a,c], and the symmetric completion proves it on [c,b].

1.2givenalgebra

For the reverse direction, choose side gauges for error ε/2. For x<c shrink the left gauge below (c−x)/2, for x>c shrink the right gauge below (x−c)/2, and at c take the minimum of the two gauges. Thus a fine cell can cross c only when tagged at c, in which case splitting it at c produces one fine cell for each side. The two side estimates then add, proving whole-interval integrability and the displayed additivity, including c=a or c=b.

2.1step 1.2algebra∎

Order u,v,w, apply step 1.2 on the two adjacent compact subintervals, and reverse any necessary limits with the orientation convention in the Statement. The resulting signed equality is the oriented three-point identity in every ordering.

Depends on

Used by

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Sources