11.14. ABSOLUTELY CONTINUOUS FUNCTIONS 347

Proposition 11.14.5 Suppose Definition 11.14.2 is unchanged except do not insist thatthe intervals be non-overlapping. Then F is not just absolutely continuous, it is also Lips-chitz. The converse also holds.

Proof: Choose m such that ∑∞n=m 2−n < δ where δ goes with 1 in the definition of abso-

lute continuity. Let r ≤ 1/2 and this implies that any such choice of r yields ∑∞n=m rn < δ .

Let Enr ≡ [F ′ > r−n] . If any Enr has measure zero, then F ′ is bounded off a set of mea-sure zero and this is what is desired. Otherwise, each Enr has a point of density. Let hn ∈[rn−1,rn−2) so r−n+1hn ≥ 1 and let r be small enough and m large enough that ∑

∞n=m hn < δ .

For tN+m a point of density for E(N+m)r let In≡ (tN+m− rhn/2, tN+m + rhn/2) . Pick N large,

say N > 9. Make r smaller if necessary so that for n ∈ [m,N +m] , m(Enr∩In)m(In)

> 12 . Note that

E(N+m)r ⊆ Enr for n < N+m and tN+m ∈ Enr must be a point of density for Enr. Then, sinceF ′ > r−n on Enr, one obtains the following sequence of inequalities.

4.5 <N +1

2=

m+N

∑n=m

12<

m+N

∑n=m

≥1︷ ︸︸ ︷r−nrhn

m(En∩ In)

m(In)=

m+N

∑n=m

r−nm(In)m(En∩ In)

m(In)=

m+N

∑n=m

r−nm(En∩ In)

≤m+N

∑n=m

∫ tN+m+rhn/2

tN+m−rhn/2XEnF ′ (t)dm≤

m+N

∑n=m

F (tN+m + rhn/2)−F (tN+m− rhn/2)< 1

by assumption, since the sum of the lengths of the intervals is smaller than δ . Thus 4.5≤ 1,a contradiction. Hence some Enr has measure zero and so F ′ is bounded by a constant Koff a set of measure zero. Hence, |F (s)−F (t)|=

∣∣∫ ts F ′ (u)du

∣∣≤ K |s− t| showing that Fis Lipschitz.

The other direction is fairly obvious. If F is Lipschitz continuous, with Lipschitz con-stant K then if ∑

mi=1 |xi+1− xi| < δ , then ∑

mi=1 |F (xi+1)−F (xi)| ≤ K ∑

mi=1 |xi+1− xi| so if

ε > 0 is given, let δ = ε/K. ■Note that when µ is the Lebesgue Stieltjes measure coming from increasing continuous

F, it follows from the definition that Dmµ (x) = limh→0F(x+h)−F(x−h)

2h . The following isanother characterization of absolute continuity.

Corollary 11.14.6 Let µ be the Lebesgue Stieltjes measure described above for in-creasing F defined on Fµ containing the Borel sets. Let I ≡ {x : Dmµ (x) = ∞} . Thenµ ≪ m on Fm ∩Fµ if and only if µ (I) has measure 0. Here Fm is the σ algebra ofLebesgue measurable sets.

Proof: ⇒ If µ ≪ m, then by Theorem 11.13.2, for all E ∈Fµ ∩Fm, it follows thatµ (E) =

∫E Dmµ (x)dm. Then by the fundamental theorem of calculus, Theorem 11.13.2,

there is a set of m measure zero N such that off this set, Dmµ (x) exists and is in R. ThusN ⊇ I and by absolute continuity, µ (I) = 0.⇐ Next suppose µ (I) = 0. Then F has no jumps because if it did, then µ (a jump)> 0

and the jump is also contained in I. Let m(E) = 0 for E a bounded set. Then define

Gn ≡{

t : lim infr→0

µ (B(t,r))2r

≤ n},n ∈ N

11.14. ABSOLUTELY CONTINUOUS FUNCTIONS 347Proposition 11.14.5 Suppose Definition 11.14.2 is unchanged except do not insist thatthe intervals be non-overlapping. Then F is not just absolutely continuous, it is also Lips-chitz. The converse also holds.Proof: Choose m such that )°_,,,2~” < 6 where 6 goes with | in the definition of abso-lute continuity. Let r < 1/2 and this implies that any such choice of r yields Y?_,,, 7” < 6.Let E,, = [F '> r"|. If any E,, has measure zero, then F ' is bounded off a set of mea-sure zero and this is what is desired. Otherwise, each FE, has a point of density. Let hy, €[r’-! r*-?) sor-"*! hy, > 1 and let r be small enough and m large enough that Y*’_,,, in < 6.For fy +m a point of density for E(y4m)r let In = (tym — Thy /2,twim + rh, /2). Pick N large,say N > 9. Make r smaller if necessary so that for n € [m,N+m], aa > 3 Note thatE\ N+m)r © E,, forn <N-+m and tyim € Enr must be a point of density for E,,,. Then, sinceF'>r™ on Ey, one obtains the following sequence of inequalities.N+1 m+N 145<—-=Y -<2 XL 2>1n+N —_——\ E AL m+N E AL m+Ny rm ppp En Vn) nn) =) r"m(h) m(En Jn) = VY r"m(E,Nh)n=m m (Un) n=m m Un) n=mM+N pty4m+rhy/2 m+N< | Lz, F! (t)dm < YF (tm+rhn/2) —F (tem —rltn/2) <1n=m J tn+m—Thn [2 n=mby assumption, since the sum of the lengths of the intervals is smaller than 6. Thus 4.5 < 1,a contradiction. Hence some E,,, has measure zero and so F’ is bounded by a constant Koff a set of measure zero. Hence, |F (s) — F (t)| =| {{ F’ (uw) du| < K|s —t| showing that Fis Lipschitz.The other direction is fairly obvious. If F is Lipschitz continuous, with Lipschitz con-stant K then if aa xi — x;| < é6, then ian |F (x41) — F (x;)| < Ky | xi —x;| so if€ > Ois given, let 6 =e/K.Note that when ju is the Lebesgue Stieltjes measure coming from increasing continuousF, it follows from the definition that D,,b (x) = limp_,o FO+n—F—h)Th . The following isanother characterization of absolute continuity.Corollary 11.14.6 Let u be the Lebesgue Stieltjes measure described above for in-creasing F defined on Fy, containing the Borel sets. Let I = {x:Dm(x) =}. ThenL<mon F;,,1Fy if and only if (1) has measure 0. Here Fy is the o algebra ofLebesgue measurable sets.Proof: = If <m, then by Theorem 11.13.2, for all E € Fy Fyn, it follows thatL(E) = fe Dm (x)dm. Then by the fundamental theorem of calculus, Theorem 11.13.2,there is a set of m measure zero N such that off this set, D,,[ (x) exists and is in R. ThusN DI and by absolute continuity, p (1) = 0.< Next suppose pu (1) = 0. Then F has no jumps because if it did, then (a jump) > 0and the jump is also contained in J. Let m(E) = 0 for E a bounded set. Then defineGy = {rating OE <a nenr>0 r