The reduced boundary of a set is a crucial concept in geometric measure theory. It provides a more regular subset of the topological boundary, essential for studying geometric properties of sets. This concept is key to understanding sets of finite perimeter.
The Federer-Volpert theorem is a cornerstone result in this field. It states that the reduced boundary of a set with finite perimeter is countably rectifiable, bridging the gap between measure theory and geometry. This theorem has far-reaching implications for studying set boundaries.
Reduced Boundary of a Set
Definition and Properties
- The reduced boundary of a set E, denoted by ∂E, is a subset of the topological boundary ∂E that satisfies certain regularity properties
- A point x belongs to the reduced boundary ∂E if and only if:
- The measure-theoretic outer unit normal νE(x) exists at x
- νE(x) is defined as the limit of the unit vectors (y - x)/|y - x| as y approaches x from outside E
- The Lebesgue density of E at x is equal to 1/2
- Lebesgue density is the limit of the ratio of the measure of E intersected with a ball centered at x to the measure of the ball, as the radius tends to zero
- The measure-theoretic outer unit normal νE(x) exists at x
Significance and Applications
- The reduced boundary provides a more regular and well-behaved subset of the topological boundary, essential for studying geometric and measure-theoretic properties of sets
- It is crucial in the formulation of:
- Gauss-Green theorem for sets of finite perimeter
- Divergence theorem for sets of finite perimeter
- Allows for the application of geometric measure theory results (area formula, coarea formula) to study properties of the reduced boundary
- Enables proving the existence of approximate tangent planes to ∂E at Hn-1-almost every point
Federer-Volpert Theorem
Statement and Rectifiability
- The Federer-Volpert theorem states that if E is a set of finite perimeter in ℝn, then:
- The reduced boundary ∂E is countably (n-1)-rectifiable
- A set is countably (n-1)-rectifiable if it can be covered, up to a set of Hn-1-measure zero, by a countable union of (n-1)-dimensional Lipschitz graphs
- Hn-1(∂E \ ∂E) = 0, where Hn-1 denotes the (n-1)-dimensional Hausdorff measure
- The reduced boundary ∂E is countably (n-1)-rectifiable
Key Steps in the Proof
- Show that the measure-theoretic outer unit normal νE(x) exists Hn-1-almost everywhere on ∂E
- Prove that the function x ↦ νE(x) is Borel measurable on ∂E
- Use the Besicovitch differentiation theorem to show that the Lebesgue density of E is equal to 1/2 at Hn-1-almost every point of ∂E
- Apply the De Giorgi structure theorem to conclude that:
- ∂E is countably (n-1)-rectifiable
- Hn-1(∂E \ ∂E) = 0
Regularity of Reduced Boundary
Implications of Federer-Volpert Theorem
- The Federer-Volpert theorem implies that the reduced boundary ∂E is (n-1)-rectifiable, indicating a certain degree of regularity
- Rectifiability allows for the application of geometric measure theory results to study properties of ∂E:
- Area formula
- Coarea formula
- The theorem can be used to prove the existence of approximate tangent planes to ∂E at Hn-1-almost every point
Measurability of the Outer Unit Normal
- The Federer-Volpert theorem implies that the measure-theoretic outer unit normal νE(x) is:
- Well-defined on ∂E
- Hn-1-measurable on ∂E
- The measurability of νE(x) is essential for studying the behavior of the perimeter measure
Reduced vs Measure-Theoretic Boundary
Definitions and Relationship
- The measure-theoretic boundary, denoted by ∂ME, is the set of points where the Lebesgue density of E is neither 0 nor 1
- The reduced boundary ∂E is a subset of the measure-theoretic boundary ∂ME
- Lebesgue density of E is equal to 1/2 at every point of ∂E
- The Federer-Volpert theorem implies that ∂E and ∂ME coincide up to a set of Hn-1-measure zero
Generalization and Importance
- The measure-theoretic boundary ∂ME can be seen as a generalization of the reduced boundary ∂E
- Allows for a more general notion of the boundary of a set in terms of Lebesgue density
- The relationship between ∂E and ∂ME is important for:
- Understanding the structure of sets of finite perimeter
- Studying the properties of the perimeter measure