Densities, essential interior and essential boundary #
Let μ be a measure on a metric space. A set s has density d at x
(TauCeti.HasDensityAt μ s x d) when the proportion μ (s ∩ closedBall x r) / μ (closedBall x r)
of s in closed balls around x tends to d as r → 0⁺. The points of density one form the
essential interior TauCeti.essentialInterior μ s, those of density zero the
essential exterior TauCeti.essentialExterior μ s, and the points of neither kind the
essential boundary TauCeti.essentialBoundary μ s. For Lebesgue measure these are the sets
E⁽¹⁾, E⁽⁰⁾ and ∂ᵉE of the theory of sets of finite perimeter.
All three sets depend only on the μ-a.e. class of s, unlike the topological interior and
frontier. They are nevertheless comparable to them: for a locally finite measure that charges
every open set, interior s ⊆ essentialInterior μ s ⊆ closure s and
essentialBoundary μ s ⊆ frontier s. For such a measure and a null-measurable set s,
complements exchange the essential interior and exterior, so the essential boundary of sᶜ is
that of s. The essential boundary of a union of any two sets lies in the union of their
essential boundaries; the same holds for an intersection of two sets one of which is
null-measurable, for any measure.
For a locally finite measure on a second-countable metric space with its Borel σ-algebra and the
Besicovitch covering property, such as a finite-dimensional real normed space, Lebesgue's density
theorem shows that the essential interior of a null-measurable set s agrees with s almost
everywhere and the essential boundary is null. The essential interior is
thus a canonical representative of the a.e. class of s.
For an additive Haar measure on a finite-dimensional real normed space of dimension n, a set
filling a proportion r ^ n ≤ c μ(s ∩ ball x r) of every small ball around x does not have
density zero at x.
Main declarations #
TauCeti.HasDensityAt μ s x d: the setshas densitydatxwith respect toμ.TauCeti.essentialInterior,TauCeti.essentialExterior,TauCeti.essentialBoundary.TauCeti.essentialInterior_congr_aeand its companions: invariance under null modification.TauCeti.essentialInterior_complandTauCeti.essentialBoundary_compl: complements.TauCeti.essentialBoundary_union_subsetandTauCeti.essentialBoundary_inter_subset.TauCeti.essentialInterior_preimage_add_rightand its companions: for a translation-invariant measure, the three sets commute with translations.TauCeti.interior_subset_essentialInterior,TauCeti.essentialInterior_subset_closureandTauCeti.essentialBoundary_subset_frontier: comparison with the topological notions.TauCeti.essentialInterior_ae_eqandTauCeti.measure_essentialBoundary: Lebesgue's density theorem.TauCeti.not_hasDensityAt_zero_of_eventually_ofReal_pow_le_mul_measure_inter_ball: a lower volume density bound against a Haar measure rules out density zero.
References #
- F. Maggi, Sets of Finite Perimeter and Geometric Variational Problems, §5.4 and §16.1.
- L. C. Evans and R. F. Gariepy, Measure Theory and Fine Properties of Functions, §1.7 and §5.8.
The set s has density d at x with respect to μ: the proportion
μ (s ∩ closedBall x r) / μ (closedBall x r) of s in the closed ball of radius r around x
tends to d as r → 0⁺.
Instances For
A density is unique.
A density is at most one.
Densities only depend on the set up to μ-null sets.
A positive density forces closed balls of small positive radius around the point to have positive finite measure: otherwise the proportions vanish.
Complements. If a null-measurable set s has density d at x, then sᶜ has density
1 - d there, provided closed balls of small positive radius around x have positive finite
measure. This holds at every point for a locally finite measure that charges every open set
(Metric.eventually_measure_closedBall_ne_zero_ne_top).
Densities only depend on the set up to μ-null sets.
Essential interior, exterior and boundary #
The essential interior of s with respect to μ: the points at which s has density
one. For Lebesgue measure this is the set E⁽¹⁾ of points of density one of E.
Instances For
The essential exterior of s with respect to μ: the points at which s has density
zero. For Lebesgue measure this is the set E⁽⁰⁾ of points of density zero of E.
Instances For
The essential boundary of s with respect to μ: the points at which s has neither
density one nor density zero. This is the measure-theoretic boundary ∂ᵉE, which ignores
modifications of E by null sets.
Instances For
The essential interior and the essential exterior are disjoint.
The essential interior is invariant under modification of the set by null sets.
The essential exterior is invariant under modification of the set by null sets.
The essential boundary is invariant under modification of the set by null sets.
Monotonicity, unions and intersections #
The essential interior is monotone, up to null sets.
The essential interior is monotone.
The essential exterior is antitone, up to null sets.
The essential exterior is antitone.
A point is in the essential exterior of a union exactly when it is in the essential exterior of both sets.
The essential boundary of a union lies in the union of the essential boundaries.
A point is in the essential interior of an intersection with a null-measurable set exactly when it is in the essential interior of both sets.
The essential boundary of an intersection with a null-measurable set lies in the union of the essential boundaries.
The essential interior of the complement of a null-measurable set is its essential exterior.
The essential exterior of the complement of a null-measurable set is its essential interior.
A null-measurable set and its complement have the same essential boundary.
Comparison with the topological interior and frontier #
A point outside the closure of s is in its essential exterior.
The essential interior of s lies in its closure.
An interior point of s is in its essential interior, for a locally finite measure that
charges every open set.
The essential exterior of s lies in the complement of its interior.
The essential boundary lies in the topological frontier, for a locally finite measure that charges every open set.
Translations #
For a translation-invariant measure, the density of the translate (· + h) ⁻¹' s at x is the
density of s at x + h.
For a translation-invariant measure, the essential interior commutes with translations.
For a translation-invariant measure, the essential exterior commutes with translations.
For a translation-invariant measure, the essential boundary commutes with translations.
Lebesgue's density theorem #
Lebesgue's density theorem. At almost every point a null-measurable set has density one or zero, according to whether the point lies in the set.
Lebesgue's density theorem. A null-measurable set agrees almost everywhere with its essential interior.
Lebesgue's density theorem. The essential exterior of a null-measurable set agrees almost everywhere with its complement.
Lebesgue's density theorem. The essential boundary of a null-measurable set is null.
The essential interior is idempotent: it is a canonical representative of the a.e. class of a null-measurable set.
Lower volume density bounds for Haar measures #
Against an additive Haar measure on a space of dimension n, a set filling a proportion
ofReal (r ^ n) ≤ c μ(s ∩ ball x r), c ≠ ∞, of every small ball around x does not have density
zero at x.