Difference between revisions of "Density of a set"
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'''Theorem 1''' | '''Theorem 1''' | ||
− | The density of a Lebesgue measurable set $E\subset \mathbb R^n$ is $1$ at $\lambda$ | + | The density of a Lebesgue measurable set $E\subset \mathbb R^n$ is $1$ at $\lambda$-a.e. $x\in E$ and $0$ at $\lambda$-a.e. $x\not \in E$. |
+ | |||
+ | The points of the first type are also called [[Density point|density points]] of $E$. | ||
===Density of a measure=== | ===Density of a measure=== | ||
Line 35: | Line 37: | ||
'''Theorem 2''' | '''Theorem 2''' | ||
− | Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$ and $\alpha$ a nonnegative real number such that the $\alpha$-dimensional density of $\mu$ exists and is positive on a set of | + | Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$ and $\alpha$ a nonnegative real number such that the $\alpha$-dimensional density of $\mu$ exists and is positive on a set of positive $\mu$-measure. Then $\alpha$ is necessarily an integer. |
====Lebesgue theorem==== | ====Lebesgue theorem==== | ||
Line 52: | Line 54: | ||
'''Theorem 4''' | '''Theorem 4''' | ||
Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$. If the $n$-dimensional density $\theta^n (\mu, x)$ exists for $\lambda$-a.e. $x$, then the measure $\mu$ is given by the formula \ref{e:densita} where $f = \theta^n (\mu, \cdot)$. | Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$. If the $n$-dimensional density $\theta^n (\mu, x)$ exists for $\lambda$-a.e. $x$, then the measure $\mu$ is given by the formula \ref{e:densita} where $f = \theta^n (\mu, \cdot)$. | ||
+ | |||
+ | The latter theorem can be generalized to Hausdorff $\alpha$-dimensional measures $\mathcal{H}^\alpha$. | ||
+ | |||
+ | '''Theorem 5''' | ||
+ | Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$. If the upper $\alpha$-dimensional density exists and it is positive and finite at $\mathcal{H}^\alpha$-a.e. $x\in \mathbb R^n$, then there is a Borel function $f$ and a Borel set $E$ with locally finite $\alpha$-dimensional Hausdorff measure such that | ||
+ | \[ | ||
+ | \mu (A) = \int_{A\cap E} f\, d\mathcal{H}^\alpha\, . | ||
+ | \] | ||
+ | |||
+ | A generalization of Theorem 3 is also possible, but much more subtle (see below). | ||
===Lower-dimensional densities of a set=== | ===Lower-dimensional densities of a set=== | ||
− | Assume $E\subset \mathbb R^n$ is a Borel set with finite $\alpha$-dimensional [[Hausdorff measure]]. The $\alpha$-dimensional upper and lower | + | Assume $E\subset \mathbb R^n$ is a [[Borel set]] with finite $\alpha$-dimensional [[Hausdorff measure]]. The $\alpha$-dimensional upper and lower densities $\theta^{\alpha, *} (E, x)$ and $\theta^\alpha_* (E,x)$ of $E$ at $x$ are defined as |
\[ | \[ | ||
− | \theta^{\alpha,*} ( | + | \theta^{\alpha,*} (E, x) := \limsup_{r\downarrow 0} \frac{\mathcal{H}^\alpha (E\cap B_r (x))}{\omega_\alpha r^\alpha} |
− | \qquad \mbox{and}\qquad \theta^\alpha_* ( | + | \qquad \mbox{and}\qquad \theta^\alpha_* (E, x) =\liminf_{r\downarrow 0} \frac{\mathcal{H}^\alpha (E \cap B_r (x))}{\omega_\alpha r^\alpha}\, . |
\] | \] | ||
− | They correspond, therefore, to the $\alpha$-dimensional densities of the Radon measure $\mu$ given by | + | They correspond, therefore, to the $\alpha$-dimensional (upper and lower) densities of the Radon measure $\mu$ given by |
\[ | \[ | ||
− | \mu (A) := \mathcal{H}^\alpha (A\cap E)\, . | + | \mu (A) := \mathcal{H}^\alpha (A\cap E)\, \qquad\mbox{for any Borel set $A\subset\mathbb R$.} |
\] | \] | ||
The following is a classical theorem in Geometric measure theory: | The following is a classical theorem in Geometric measure theory: | ||
− | '''Theorem | + | '''Theorem 6''' |
− | If $E\subset \mathbb R^n$ is a Borel set with finite $\alpha$-dimensional | + | If $E\subset \mathbb R^n$ is a Borel set with finite $\alpha$-dimensional Hausdorff measure, then |
* $\theta^{\alpha,*} (E, x) =0$ for $\mathcal{H}^\alpha$-a.e. $x\not\in E$. | * $\theta^{\alpha,*} (E, x) =0$ for $\mathcal{H}^\alpha$-a.e. $x\not\in E$. | ||
− | * $1\geq \theta^\alpha_* (E,x) \geq 2^{-\alpha}$ for $\mathcal{H}^\alpha$ | + | * $1\geq \theta^\alpha_* (E,x) \geq 2^{-\alpha}$ for $\mathcal{H}^\alpha$-a.e. $x\in E$. |
+ | ====Besicovitch-Preiss theorem and rectifiability==== | ||
+ | However the existence of the density fails in general: as a consequence of Marstrand's Theorem 2 the existence of a nontrivial $\alpha$-dimensional | ||
+ | density implies that $\alpha$ is an integer. But even in the case when $\alpha$ is an integer, it was discovered by Besicovitch that the density does | ||
+ | not necessarily exist. Indeed the following generalization of Besicovitch's theorem was achieved by Preiss in the mid eighties: | ||
− | '' | + | '''Theorem 7''' |
+ | Let $E\subset \mathbb R^n$ be a Borel set with positive and finite $k$-dimensional Hausdorff measure, where $k\in \mathbb N$. The $k$-dimensional density | ||
+ | exists at $\mathcal{H}^k$-a.e. $x\in E$ if and only if the set $E$ is [[Rectifiable set|rectifiable]], i.e. if there are countably many $C^1$ $k$-dimensional submanifolds | ||
+ | of $\mathbb R^n$ which cover $\mathcal{H}^k$-almost all $E$. | ||
− | + | For non-rectifiable sets $E$ the lower-dimensional density might display a variety of different behavior. Besicovitch proved that for $1$-dimensional non-rectifiable sets | |
+ | the lower dimensional density cannot be larger than $\frac{3}{4}$ and advanced the following long-standing conjecture. | ||
− | + | '''Conjecture 8''' | |
+ | Let $E\subset \mathbb R^n$ be a Borel set with positive and finite $1$-dimensional Hausdorff measure. If $\theta^1_* (E, x)>\frac{1}{2}$ for $\mathcal{H}^1$-a.e. | ||
+ | $x\in E$, then the set $E$ is rectifiable. | ||
− | + | Besicovitch's $\frac{3}{4}$ treshold has been improved by Preiss and Tiser in {{Cite|PT}}. | |
− | === | + | ===Besicovitch-Marstrand-Preiss Theorem=== |
− | + | Combining the various theorems exposed so far we reach the following characterization of measures $\mu$ for which densities exist and are nontrivial | |
+ | almost everywhere. | ||
+ | '''Theorem 9''' | ||
+ | Let $\mu$ be a locally finite Radon measure and $\alpha$ a nonnegative real number. Then $\theta^\alpha (\mu, x)$ exists, it is finite and positive | ||
+ | at $\mu$-a.e. $x\in \mathbb R^n$ if and only $\alpha$ is an integer $k$ and there are a rectifiable $k$-dimensional Borel set $E$ and a Borel function $f: E\to ]0, \infty[$ such that | ||
+ | \[ | ||
+ | \mu (A) = \int_{A\cap E} f\, d\mathcal{H}^k\qquad \mbox{for any Borel $E\subset \mathbb R^n$.} | ||
+ | \] | ||
+ | Moreover, in this case $\theta^k (E,x)=f(x)$ for $\mathcal{H}^k$-a.e. $x\in E$ and $\theta^k (E, x) =0$ for $\mathcal{H}^k$-a.e. $x\not\in E$. | ||
+ | ====Comments==== | ||
+ | See {{Cite|Ta}} for a nice topological application of the classical notion of Lebesgue density. | ||
− | + | The definition of $\alpha$-dimensional density of a Radon measure can be generalized to metric spaces. In general, however, very little is known outside of the Euclidean setting. | |
− | |||
====References==== | ====References==== | ||
− | + | {| | |
+ | |- | ||
+ | |valign="top"|{{Ref|AFP}}|| L. Ambrosio, N. Fusco, D. Pallara, "Functions of bounded variations and free discontinuity problems". Oxford Mathematical Monographs. The Clarendon Press, Oxford University Press, New York, 2000. {{MR|1857292}}{{ZBL|0957.49001}} | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Be}}|| S. Besicovitch, "On the fundamental geometrical properties of linearly measurable plane sets of points II", ''Math. Ann.'', '''115''' (1938), pp. 296–329. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|De}}|| C. De Lellis, "Rectifiable sets, densities and tangent measures" Zurich Lectures in Advanced Mathematics. European Mathematical Society (EMS), Zürich, 2008. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Fe}}|| H. Federer, "Geometric measure theory". Volume 153 of Die Grundlehren der mathematischen Wissenschaften. Springer-Verlag New York Inc., New York, 1969. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Mar}}|| J. M. Marstrand, "The (φ, s) regular subset of n space". ''Trans. Amer. Math. Soc.'', '''113''' (1964), pp. 369–392. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Ma}}|| P. Mattila, "Geometry of sets and measures in euclidean spaces". Cambridge Studies in Advanced Mathematics, 44. Cambridge University Press, Cambridge, 1995. {{MR|1333890}} {{ZBL|0911.28005}} | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Pr}}|| D. Preiss, "Geometry of measures in $\mathbb R^n$ : distribution, rectifiability, and densities". ''Ann. of Math.'', '''125''' (1987), pp. 537–643. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|PT}}|| D. Preiss, J. Tiser, "On Besicovitch’s $\frac{1}{2}$-problem. ''J. London Math. Soc. (2)'', '''45''' (1992), pp. 279–287. | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Ta}}|| F.D. Tall, "The density topology" ''Pacific J. Math'' , '''62''' (1976) pp. 275–284 | ||
+ | |- | ||
+ | |} |
Revision as of 08:05, 3 August 2012
2020 Mathematics Subject Classification: Primary: 28A33 Secondary: 49Q15 [MSN][ZBL]
A concept of classical measure theory generalized further in Geometric measure theory
Lebesgue density of a set
Given a Lebesgue measurable set $E$ in the standard Euclidean space $\mathbb R^n$ and a point $x\in\mathbb R^n$, the upper and lower densities of $E$ at $x$ are defined respectively as \[ \limsup_{r\downarrow 0} \frac{\lambda (B_r (x)\cap E)}{\omega_n r^n} \qquad \mbox{and} \qquad \liminf_{r\downarrow 0} \frac{\lambda (B_r (x)\cap E)}{\omega_n r^n}\, , \] where $\lambda$ denotes the Lebesgue measure and $\omega_n$ the volume of the unit $n$-dimensional ball. If the two numbers coincides, i.e. if the following limit exists, \[ \lim_{r\downarrow 0} \frac{\lambda (B_r (x)\cap E)}{\omega_n r^n}\, , \] the resulting number is called the density of $E$ at $x$. The following is a classical result in measure theory, due to Lebesgue in the case $n=1$:
Theorem 1 The density of a Lebesgue measurable set $E\subset \mathbb R^n$ is $1$ at $\lambda$-a.e. $x\in E$ and $0$ at $\lambda$-a.e. $x\not \in E$.
The points of the first type are also called density points of $E$.
Density of a measure
The concept above has been generalized in geometric measure theory to measures, starting from the work of Besicovitch. Consider a (locally finite) Radon measure $\mu$ in the Euclidean space $\mathbb R^n$, a point $x\in \mathbb R^n$ and a nonnegative real number $\alpha$. The $\alpha$-dimensional upper and lower densities of $\mu$ at $x$ are defined as \[ \theta^{\alpha,*} (\mu, x) := \limsup_{r\downarrow 0} \frac{\mu (B_r (x))}{\omega_\alpha r^\alpha} \qquad \mbox{and}\qquad \theta^\alpha_* (\mu, x) =\liminf_{r\downarrow 0} \frac{\mu (B_r (x))}{\omega_\alpha r^\alpha}\, , \] where the normalizing factor $\omega_\alpha$ is the $\alpha$-dimensional volume of the unit ball in $\mathbb R^\alpha$ when $\alpha$ is a positive integer and in general $\omega_\alpha = \pi^{\alpha/2} \Gamma (1+\alpha/2)$. If the two numbers coincide, the resulting value is called the $\alpha$-dimensional density of $\mu$ at $x$. The following Theorem by Marstrand shows that the density might exist and be nontrivial if and only if $\alpha$ is an integer.
Theorem 2 Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$ and $\alpha$ a nonnegative real number such that the $\alpha$-dimensional density of $\mu$ exists and is positive on a set of positive $\mu$-measure. Then $\alpha$ is necessarily an integer.
Lebesgue theorem
Concerning $n$-dimensional densities, the following theorem corresponds to the fact that, given a summable function $f$, $\lambda$-a.e. point $x$ is a Lebesgue point for $f$:
Theorem 3 Let $f\in L^1_{loc} (\mathbb R^n)$ and consider the measure \begin{equation}\label{e:densita} \mu (A):= \int_A f\, d\lambda\, . \end{equation} Then the $n$--dimensional density of $\mu$ exists at $\lambda$--a.e. $x\in \mathbb R^n$ and coincides with $f(x)$.
The converse is also true and is a particular case of a more general result on the Differentiation of measures:
Theorem 4 Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$. If the $n$-dimensional density $\theta^n (\mu, x)$ exists for $\lambda$-a.e. $x$, then the measure $\mu$ is given by the formula \ref{e:densita} where $f = \theta^n (\mu, \cdot)$.
The latter theorem can be generalized to Hausdorff $\alpha$-dimensional measures $\mathcal{H}^\alpha$.
Theorem 5 Let $\mu$ be a locally finite Radon measure on $\mathbb R^n$. If the upper $\alpha$-dimensional density exists and it is positive and finite at $\mathcal{H}^\alpha$-a.e. $x\in \mathbb R^n$, then there is a Borel function $f$ and a Borel set $E$ with locally finite $\alpha$-dimensional Hausdorff measure such that \[ \mu (A) = \int_{A\cap E} f\, d\mathcal{H}^\alpha\, . \]
A generalization of Theorem 3 is also possible, but much more subtle (see below).
Lower-dimensional densities of a set
Assume $E\subset \mathbb R^n$ is a Borel set with finite $\alpha$-dimensional Hausdorff measure. The $\alpha$-dimensional upper and lower densities $\theta^{\alpha, *} (E, x)$ and $\theta^\alpha_* (E,x)$ of $E$ at $x$ are defined as \[ \theta^{\alpha,*} (E, x) := \limsup_{r\downarrow 0} \frac{\mathcal{H}^\alpha (E\cap B_r (x))}{\omega_\alpha r^\alpha} \qquad \mbox{and}\qquad \theta^\alpha_* (E, x) =\liminf_{r\downarrow 0} \frac{\mathcal{H}^\alpha (E \cap B_r (x))}{\omega_\alpha r^\alpha}\, . \] They correspond, therefore, to the $\alpha$-dimensional (upper and lower) densities of the Radon measure $\mu$ given by \[ \mu (A) := \mathcal{H}^\alpha (A\cap E)\, \qquad\mbox{for any Borel set '"`UNIQ-MathJax81-QINU`"'.} \] The following is a classical theorem in Geometric measure theory:
Theorem 6 If $E\subset \mathbb R^n$ is a Borel set with finite $\alpha$-dimensional Hausdorff measure, then
- $\theta^{\alpha,*} (E, x) =0$ for $\mathcal{H}^\alpha$-a.e. $x\not\in E$.
- $1\geq \theta^\alpha_* (E,x) \geq 2^{-\alpha}$ for $\mathcal{H}^\alpha$-a.e. $x\in E$.
Besicovitch-Preiss theorem and rectifiability
However the existence of the density fails in general: as a consequence of Marstrand's Theorem 2 the existence of a nontrivial $\alpha$-dimensional density implies that $\alpha$ is an integer. But even in the case when $\alpha$ is an integer, it was discovered by Besicovitch that the density does not necessarily exist. Indeed the following generalization of Besicovitch's theorem was achieved by Preiss in the mid eighties:
Theorem 7 Let $E\subset \mathbb R^n$ be a Borel set with positive and finite $k$-dimensional Hausdorff measure, where $k\in \mathbb N$. The $k$-dimensional density exists at $\mathcal{H}^k$-a.e. $x\in E$ if and only if the set $E$ is rectifiable, i.e. if there are countably many $C^1$ $k$-dimensional submanifolds of $\mathbb R^n$ which cover $\mathcal{H}^k$-almost all $E$.
For non-rectifiable sets $E$ the lower-dimensional density might display a variety of different behavior. Besicovitch proved that for $1$-dimensional non-rectifiable sets the lower dimensional density cannot be larger than $\frac{3}{4}$ and advanced the following long-standing conjecture.
Conjecture 8 Let $E\subset \mathbb R^n$ be a Borel set with positive and finite $1$-dimensional Hausdorff measure. If $\theta^1_* (E, x)>\frac{1}{2}$ for $\mathcal{H}^1$-a.e. $x\in E$, then the set $E$ is rectifiable.
Besicovitch's $\frac{3}{4}$ treshold has been improved by Preiss and Tiser in [PT].
Besicovitch-Marstrand-Preiss Theorem
Combining the various theorems exposed so far we reach the following characterization of measures $\mu$ for which densities exist and are nontrivial almost everywhere.
Theorem 9 Let $\mu$ be a locally finite Radon measure and $\alpha$ a nonnegative real number. Then $\theta^\alpha (\mu, x)$ exists, it is finite and positive at $\mu$-a.e. $x\in \mathbb R^n$ if and only $\alpha$ is an integer $k$ and there are a rectifiable $k$-dimensional Borel set $E$ and a Borel function $f: E\to ]0, \infty[$ such that \[ \mu (A) = \int_{A\cap E} f\, d\mathcal{H}^k\qquad \mbox{for any Borel '"`UNIQ-MathJax126-QINU`"'.} \] Moreover, in this case $\theta^k (E,x)=f(x)$ for $\mathcal{H}^k$-a.e. $x\in E$ and $\theta^k (E, x) =0$ for $\mathcal{H}^k$-a.e. $x\not\in E$.
Comments
See [Ta] for a nice topological application of the classical notion of Lebesgue density.
The definition of $\alpha$-dimensional density of a Radon measure can be generalized to metric spaces. In general, however, very little is known outside of the Euclidean setting.
References
[AFP] | L. Ambrosio, N. Fusco, D. Pallara, "Functions of bounded variations and free discontinuity problems". Oxford Mathematical Monographs. The Clarendon Press, Oxford University Press, New York, 2000. MR1857292Zbl 0957.49001 |
[Be] | S. Besicovitch, "On the fundamental geometrical properties of linearly measurable plane sets of points II", Math. Ann., 115 (1938), pp. 296–329. |
[De] | C. De Lellis, "Rectifiable sets, densities and tangent measures" Zurich Lectures in Advanced Mathematics. European Mathematical Society (EMS), Zürich, 2008. |
[Fe] | H. Federer, "Geometric measure theory". Volume 153 of Die Grundlehren der mathematischen Wissenschaften. Springer-Verlag New York Inc., New York, 1969. |
[Mar] | J. M. Marstrand, "The (φ, s) regular subset of n space". Trans. Amer. Math. Soc., 113 (1964), pp. 369–392. |
[Ma] | P. Mattila, "Geometry of sets and measures in euclidean spaces". Cambridge Studies in Advanced Mathematics, 44. Cambridge University Press, Cambridge, 1995. MR1333890 Zbl 0911.28005 |
[Pr] | D. Preiss, "Geometry of measures in $\mathbb R^n$ : distribution, rectifiability, and densities". Ann. of Math., 125 (1987), pp. 537–643. |
[PT] | D. Preiss, J. Tiser, "On Besicovitch’s $\frac{1}{2}$-problem. J. London Math. Soc. (2), 45 (1992), pp. 279–287. |
[Ta] | F.D. Tall, "The density topology" Pacific J. Math , 62 (1976) pp. 275–284 |
Density of a set. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Density_of_a_set&oldid=27341