Hausdorff measure

Jordan Bell
October 29, 2014

1 Outer measures and metric outer measures

Suppose that X is a set. A function ν:𝒫⁢(X)→[0,∞] is said to be an outer measure if (i) ν⁢(∅)=0, (ii) ν⁢(A)≤ν⁢(B) when A⊂B, and, (iii) for any countable collection {Aj}⊂𝒫⁢(X),

ν⁢(⋃j=1∞Aj)≤∑j=1∞ν⁢(Aj).

We say that a subset A of X is ν-measurable if

ν⁢(E)=ν⁢(E∩A)+ν⁢(E∩Ac),E∈𝒫⁢(X). (1)

Here, instead of taking a σ-algebra as given and then defining a measure on this σ-algebra (namely, on the measurable sets), we take an outer measure as given and then define measurable sets using this outer measure. Carathéodory’s theorem11 1 Gerald B. Folland, Real Analysis, second ed., p. 29, Theorem 1.11. states that the collection ℳ of ν-measurable sets is a σ-algebra and that the restriction of ν to ℳ is a complete measure.

Suppose that (X,ρ) is a metric space. An outer measure ν on X is said to be a metric outer measure if

ρ⁢(A,B)=inf⁡{ρ⁢(a,b):a∈A,b∈B}>0

implies that

ν⁢(A∪B)=ν⁢(A)+ν⁢(B).

We prove that the Borel sets are ν-measurable.22 2 Gerald B. Folland, Real Analysis, second ed., p. 349, Proposition 11.16. That is, we prove that the Borel σ-algebra is contained in the σ-algebra of ν-measurable sets.

Theorem 1.

If ν is a metric outer measure on a metric space (X,ρ), then every Borel set is ν-measurable.

Proof.

Because ν is an outer measure, by Carathéodory’s theorem the collection ℳ of ν-measurable sets is a σ-algebra, and hence to prove that ℳ contains the Borel σ-algebra it suffices to prove that ℳ contains all the closed sets. Let F be a closed set in X, and let E be a subset of X. Because ν is an outer measure,

ν⁢(E)=ν⁢((E∩F)∪(E∩Fc))≤ν⁢(E∩F)+ν⁢(E∩Fc).

In the case ν⁢(E)=∞, certainly ν⁢(E)≥ν⁢(E∩F)+ν⁢(E∩Fc). In the case ν⁢(E)<∞, for each n let

En={x∈E∖F:ρ⁢(x,F)≥n-1},

which satisfies ρ⁢(En,F)≥n-1. Because ρ⁢(En,E∩F)≥ρ⁢(En,F)≥n-1, the fact that ν is a metric outer measure tells us that

ν⁢((E∩F)∪En)=ν⁢(E∩F)+ν⁢(En). (2)

Because F is closed, for any x∈E∖F we have ρ⁢(x,F)>0, and hence

E∖F=⋃n=1∞En. (3)

Therefore

E=(E∩F)∪(E∩Fc)=(E∩F)∪⋃n=1∞En=⋃n=1∞((E∩F)∪En),

hence for each n, using this and (2) we have

ν⁢(E)≥ν⁢((E∩F)∪En)=ν⁢(E∩F)+ν⁢(En).

To prove that ν⁢(E)≥ν⁢(E∩F)+ν⁢(E∩Fc), it now suffices to prove that

limn→∞⁡ν⁢(En)=ν⁢(E∩Fc).

Let Dn=En+1∖En. For x∈Dn+1 and y∈X satisfying ρ⁢(x,y)<((n+1)⁢n)-1, we have

ρ⁢(y,F)≤ρ⁢(x,y)+ρ⁢(x,F)<1n⁢(n+1)+1n+1=1n,

which implies that y∉En. Thus,

ρ⁢(Dn+1,En)≥1n⁢(n+1). (4)

For any n, using (4) and the fact that ν is a metric outer measure,

ν⁢(E2⁢n+1) = ν⁢(D2⁢n∪E2⁢n)
≥ ν⁢(D2⁢n∪E2⁢n-1)
= ν⁢(D2⁢n)+ν⁢(E2⁢n-1)
≥ ⋯
= ν⁢(D2⁢n)+ν⁢(D2⁢n-2)+⋯+ν⁢(D2)+ν⁢(E1)
≥ ∑j=1nν⁢(D2⁢j),

and

ν⁢(E2⁢n) = ν⁢(D2⁢n-1∪E2⁢n-1)
≥ ν⁢(D2⁢n-1∪E2⁢n-2)
= ν⁢(D2⁢n-1)+ν⁢(E2⁢n-2)
≥ ⋯
= ν⁢(D2⁢n-1)+ν⁢(D2⁢n-3)+⋯+ν⁢(D3)+ν⁢(D1)+ν⁢(E0)
= ∑j=1nν⁢(D2⁢j-1).

But En⊂E so ν⁢(En)≤ν⁢(E), and hence each of the series ∑j=1∞ν⁢(D2⁢j) and ∑j=1∞ν⁢(D2⁢j-1) converges to a value ≤ν⁢(E). Thus the series ∑j=1∞ν⁢(Dj) converges to a value ≤2⁢ν⁢(E). But for any n,

ν⁢(E∖F)=ν⁢(En∪⋃j=n∞Dj)≤ν⁢(En)+∑j=n∞ν⁢(Dj).

Because the series ∑j=1∞ν⁢(Dj) converges, the sum on the right-hand side of the above tends to 0 as n→∞, so

ν⁢(E∖F)≤lim infn→∞⁡ν⁢(En)≤lim supn→∞⁡ν⁢(En)≤ν⁢(E∖F);

the last inequality is due to (3), which tells us ν⁢(En)≤ν⁢(E∖F). Therefore,

limn→∞⁡ν⁢(En)=ν⁢(E∖F)=ν⁢(E∩Fc),

which completes the proof. ∎

We shall use the following.33 3 Gerald B. Folland, Real Analysis, second ed., p. 29, Proposition 1.10.

Lemma 2.

Let (X,ρ) be a metric space. Suppose that ℰ⊂𝒫⁢(X) satisfies ∅,X∈ℰ and that d:ℰ→[0,∞] satisfies d⁢(∅)=0. Then the function ν:𝒫⁢(X)→[0,∞] defined by

ν⁢(A)=inf⁡{∑j=1∞d⁢(Ej):Ej∈ℰ⁢ and ⁢A⊂⋃j=1∞Ej},A∈𝒫⁢(X)

is an outer measure.

We remark that if there is no covering of a set A by countably many elements of ℰ then ν⁢(A) is an infinimum of an empty set and is thus equal to ∞.

2 Hausdorff measure

Suppose that (X,ρ) is a metric space and let p≥0, δ>0. Let ℰ be the collection of those subsets of X with diameter ≤δ together with the set X, and define d⁢(A)=(diam⁢A)p. By Lemma 2, the function Hp,δ:𝒫⁢(X)→[0,∞] defined by

Hp,δ⁢(A)=inf⁡{∑j=1∞d⁢(Ej):Ej∈ℰ and A⊂⋃j=1∞Ej},A∈𝒫⁢(X)

is an outer measure. If δ1≤δ2 then Hp,δ1⁢(A)≥Hp,δ2⁢(A), from which it follows that for each A∈𝒫⁢(X), as δ tends to 0, Hp,δ⁢(A) tends to some element of [0,∞]. We define Hp=limδ→0⁡Hp,δ and show that this is a metric outer measure.44 4 Gerald B. Folland, Real Analysis, second ed., p. 350, Proposition 11.17.

Theorem 3.

Suppose that (X,ρ) is a metric space and let p≥0. Then Hp:𝒫⁢(X)→[0,∞] defined by

Hp⁢(A)=limδ→0⁡Hp,δ⁢(A),A∈𝒫⁢(X).

is a metric outer measure.

Proof.

First we establish that Hp is an outer measure. It is apparent that Hp⁢(∅)=0. If A⊂B, then, using that Hp,δ is a metric outer measure,

Hp⁢(A)=limδ→0⁡Hp,δ⁢(A)≤limδ→0⁡Hp,δ⁢(B)=Hp⁢(B).

If {Aj}⊂𝒫⁢(X) is countable then, using that Hp,δ is a metric outer measure,

Hp⁢(⋃j=1∞Aj) =limδ→0⁡Hp,δ⁢(⋃j=1∞Aj)
≤limδ→0⁡∑j=1∞Hp,δ⁢(Aj)
=∑j=1∞limδ→0⁡Hp,δ⁢(Aj)
=∑j=1∞Hp⁢(Aj).

Hence Hp is an outer measure.

To obtain that Hp is a metric outer measure, we must show that if ρ⁢(A,B)>0 then Hp⁢(A∪B)≥Hp⁢(A)+Hp⁢(B). Let 0<δ<ρ⁢(A,B) and let ℰ be the collection of those subsets of X with diameter ≤δ together with the set X. If there is no covering of A∪B by countably many elements of ℰ, then Hp⁢(A∪B)≥Hp,δ⁢(A∪B)=∞. Otherwise, let {Ej}⊂ℰ be a covering of A∪B. For each j, because diam⁢Ej≤δ<ρ⁢(A,B), it follows that Ej does not intersect both A and B. Write

ℰ={Eaj}∪{Ebj},

where Eaj∩B=∅ and Ebj∩A=∅. Then A⊂⋃Eaj and B⊂⋃Ebj, so

∑j=1∞(diam⁢Ej)p=∑j=1∞(diam⁢Eaj)p+∑j=1∞(diam⁢Ejb)p≥Hp,δ⁢(A)+Hp,δ⁢(B).

This is true for any covering of A∪B by countably many element of ℰ, so

Hp,δ⁢(A∪B)≥Hp,δ⁢(A)+Hp,δ⁢(B).

The above inequality is true for any 0<δ<ρ⁢(A,B), and taking δ→0 yields

Hp⁢(A∪B)≥Hp⁢(A)+Hp⁢(B),

completing the proof. ∎

We call the metric outer measure Hp:𝒫⁢(X)→[0,∞] in the above theorem the p-dimensional Hausdorff outer measure. From Theorem 1 it follows that the restriction of Hp to the Borel σ-algebra ℬX of a metric space is a meausure. We call this restriction the p-dimensional Hausdorff measure, and denote it also by Hp.

It is straightforward to verify that if T:X→X is an isometric isomorphism then Hp∘T=Hp. In particular, for X=ℝn, Hp is invariant under translations.

We will use the following inequality when talking about Hausdorff measure on ℝn.55 5 Gerald B. Folland, Real Analysis, second ed., p. 350, Proposition 11.18.

Lemma 4.

Let Y be a set and (X,ρ) be a metric space. If f,g:Y→X satisfy

ρ⁢(f⁢(y),f⁢(z))≤C⁢ρ⁢(g⁢(y),g⁢(z)),y,z∈Y,

then for any A∈𝒫⁢(Y),

Hp⁢(f⁢(A))≤Cp⁢Hp⁢(g⁢(A)).
Proof.

Take δ>0 and ϵ>0. There are countably many sets Ej that cover g⁢(A) each with diameter ≤C-1⁢δ and such that

∑(diam⁢Ej)p≤Hp⁢(g⁢(A))+ϵ.

Let a∈A. There is some j with g⁢(a)∈Ej, so a∈g-1⁢(Ej) and then f⁢(a)∈f⁢(g-1⁢(Ej)). Therefore the sets f⁢(g-1⁢(Ej)) cover f⁢(A). For u,v∈f⁢(g-1⁢(Ej)), there are y,z∈g-1⁢(Ej) with u=f⁢(y),v=f⁢(z). Because g⁢(y),g⁢(z)∈Ej,

ρ⁢(u,v)=ρ⁢(f⁢(y),f⁢(z))≤C⁢ρ⁢(g⁢(y),g⁢(z))≤C⁢diam⁢Ej,

hence

diam⁢f⁢(g-1⁢(Ej))≤C⁢diam⁢Ej.

Since the sets f⁢(g-1⁢(Ej)) cover f⁢(A) and each has diameter ≤C⁢diam⁢Ej≤δ,

Hp,δ⁢(f⁢(A))≤∑(diam⁢f⁢(g-1⁢(Ej)))p≤∑Cp⁢(diam⁢Ej)p≤Cp⁢(Hp⁢(g⁢(A))+ϵ).

This is true for all δ>0, so taking δ→0,

Hp⁢(f⁢(A))≤Cp⁢(Hp⁢(g⁢(A))+ϵ).

This is true for all ϵ>0, so taking ϵ→0,

Hp⁢(f⁢(A))≤Cp⁢Hp⁢(g⁢(A)).

∎

3 Hausdorff dimension

Theorem 5.

If Hp⁢(A)<∞ then Hq⁢(A)=0 for all q>p.

Proof.

Let δ>0. Then Hp,δ⁢(A)≤Hp⁢(A)<∞ Let {Ej} be countably many sets each with diameter ≤δ such that A⊂⋃Ej and

∑(diam⁢Ej)p≤Hp,δ⁢(A)+1≤Hp⁢(A)+1.

This gives us

Hq.δ⁢(A)≤∑(diam⁢Ej)q =∑(diam⁢Ej)q-p⁢(diam⁢Ej)p
≤δq-p⁢∑(diam⁢Ej)p
≤δq-p⁢(Hp⁢(A)+1).

This is true for any δ>0 and q-p>0, so taking δ→0 we obtain Hq⁢(A)=0. ∎

For A∈𝒫⁢(X), we define the Hausdorff dimension of A to be

inf⁡{q≥0:Hq⁢(A)=0}.

If the set whose infimum we are taking is empty, then the Hausdorff dimension of A is ∞.

4 Radon measures and Haar measures

Before speaking about Hausdorff measure on ℝn, we remind ourselves of some material about Radon measures and Haar measures. Let X be a locally compact Hausdorff space. A Borel measure μ on X is said to be a Radon measure if (i) it is finite on each compact set, (ii) for any Borel set E,

μ⁢(E)=inf⁡{μ⁢(U):U open and E⊂U},

and (iii) for any open set E,

μ⁢(E)=sup⁡{μ⁢(K):K compact and K⊂E}.

It is a fact that if X is a locally compact Hausdorff space in which every open set is σ-compact, then every Borel measure on X that is finite on compact sets is a Radon measure.66 6 Gerald B. Folland, Real Analysis, second ed., p. 217, Theorem 7.8.

Suppose that G is a locally compact group. A Borel measure μ on G is said to be left-invariant if for all x∈G and E∈ℬG,

μ⁢(x⁢E)=μ⁢(E).

A left Haar measure on G is a nonzero left-invariant Radon measure on G. It is a fact that if μ and ν are left Haar measures on G then there is some c>0 such that μ=c⁢ν.77 7 Gerald B. Folland, Real Analysis, second ed., p. 344, Theorem 11.9.

5 Hausdorff measure in Rn

Let mn denote Lebesgue measure on ℝn.

Lemma 6.

If E is a Borel set in ℝn, then

Hn⁢(E)≥2n⁢mn⁢(E).
Proof.

Let ϵ>0 and let {Ej} be countably many closed sets that cover E and such that

∑(diam⁢Ej)n≤Hn⁢(E)+ϵ.

The isodiametric inequality (which one proves using the Brunn-Minkowski inequality) states that if A is a Borel set in ℝn, then

mn⁢(A)≤(diam⁢A2)n.

Using this gives

∑2n⁢mn⁢(Ej)≤Hn⁢(E)+ϵ.

But because the sets Ej cover E we have mn⁢(E)≤mn⁢(⋃Ej)≤∑mn⁢(Ej), so we get

mn⁢(E)≤Hn⁢(E)+ϵ2n.

This expression does not involve the sets Ej (which depend on ϵ), and since this expression is true for any ϵ>0, taking ϵ→0 yields

mn⁢(E)≤Hn⁢(E)2n.

∎

Let

Q={x∈ℝn:|x1|≤12,…,|xn|≤12}.
Lemma 7.

0<Hn⁢(Q)<∞.

Proof.

For any m≥1, the cube Q can be covered by mn cubes q1,…,qmn of side length 1m. Let 0<δ<1 and let m>1δ. The distance from the center of qj to one of the vertices of qj is

r=(12⁢m)2+⋯+(12⁢m)2=n2⁢m.

Inscribe qj in a closed ball bj with the same center as qj and radius r. These balls cover Q. Hence

Hp,δ⁢(Q)≤∑j=1mn(diam⁢bj)n=∑j=1mn(2⁢r)n=(2⁢r)n⋅mn=nn/2.

Taking δ→0 gives Hp⁢(Q)≤nn/2<∞.

On the other hand, by Lemma 6,

Hn⁢(Q)≥2n⁢mn⁢(Q)=2n>0.

∎

Theorem 8.

There is some constant cn>0 such that

Hn=cn⁢mn.
Proof.

ℝn is a locally compact Hausdorff space in which every open set in ℝn is σ-compact. Therefore, to show that Hn is a Radon measure it suffices to show that Hn is finite on every compact set. If K is a compact subset of ℝn, there is some r>0 such that K⊂r⁢Q. By Lemma 4 and Lemma 7 we get Hn⁢(r⁢Q)<∞, so Hn⁢(K)<∞. Therefore Hn is a Radon measure.

Because Hn⁢(Q)>0, Hn is not the zero measure. Any translation is an isometric isomorphism ℝn→ℝn, so Hn is invariant under translations. Thus Hn is a left Haar measure on ℝn. But Lebesgue measure mn is also a left Haar measure on ℝn, so there is some cn>0 such that

Hn=cn⁢mn,

proving the claim. ∎