Hausdorff density explained

In measure theory, a field of mathematics, the Hausdorff density measures how concentrated a Radon measure is at some point.

Definition

Let

\mu

be a Radon measure and

a\inRn

some point in Euclidean space. The s-dimensional upper and lower Hausdorff densities are defined to be, respectively,

\Theta*s(\mu,a)=\limsupr

\mu(Br(a))
rs
and
s
\Theta
*

(\mu,a)=\liminfr

\mu(Br(a))
rs
where

Br(a)

is the ball of radius r > 0 centered at a. Clearly,
s
\Theta
*

(\mu,a)\leq\Theta*s(\mu,a)

for all

a\inRn

. In the event that the two are equal, we call their common value the s-density of

\mu

at a and denote it

\Thetas(\mu,a)

.

Marstrand's theorem

The following theorem states that the times when the s-density exists are rather seldom.

Marstrand's theorem: Let

\mu

be a Radon measure on

Rd

. Suppose that the s-density

\Thetas(\mu,a)

exists and is positive and finite for a in a set of positive

\mu

measure. Then s is an integer.

Preiss' theorem

In 1987 David Preiss proved a stronger version of Marstrand's theorem. One consequence is that sets with positive and finite density are rectifiable sets.

Preiss' theorem: Let

\mu

be a Radon measure on

Rd

. Suppose that m

\geq1

is an integer and the m-density

\Thetam(\mu,a)

exists and is positive and finite for

\mu

almost every a in the support of

\mu

. Then

\mu

is m-rectifiable, i.e.

\mu\llHm

(

\mu

is absolutely continuous with respect to Hausdorff measure

Hm

) and the support of

\mu

is an m-rectifiable set.

External links

References