Measure (mathematics)

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Short description: Generalization of mass, length, area and volume
Informally, a measure has the property of being monotone in the sense that if [math]\displaystyle{ A }[/math] is a subset of [math]\displaystyle{ B, }[/math] the measure of [math]\displaystyle{ A }[/math] is less than or equal to the measure of [math]\displaystyle{ B. }[/math] Furthermore, the measure of the empty set is required to be 0.

In mathematics, the concept of a measure is a generalization and formalization of geometrical measures (length, area, volume) and other common notions, such as mass and probability of events. These seemingly distinct concepts have many similarities and can often be treated together in a single mathematical context. Measures are foundational in probability theory, integration theory, and can be generalized to assume negative values, as with electrical charge. Far-reaching generalizations (such as spectral measures and projection-valued measures) of measure are widely used in quantum physics and physics in general.

The intuition behind this concept dates back to Ancient Greece, when Archimedes tried to calculate the area of a circle. But it was not until the late 19th and early 20th centuries that measure theory became a branch of mathematics. The foundations of modern measure theory were laid in the works of Émile Borel, Henri Lebesgue, Nikolai Luzin, Johann Radon, Constantin Carathéodory, and Maurice Fréchet, among others.

Definition

Countable additivity of a measure [math]\displaystyle{ \mu }[/math]: The measure of a countable disjoint union is the same as the sum of all measures of each subset.

Let [math]\displaystyle{ X }[/math] be a set and [math]\displaystyle{ \Sigma }[/math] a [math]\displaystyle{ \sigma }[/math]-algebra over [math]\displaystyle{ X. }[/math] A set function [math]\displaystyle{ \mu }[/math] from [math]\displaystyle{ \Sigma }[/math] to the extended real number line is called a measure if it satisfies the following properties:

  • Non-negativity: For all [math]\displaystyle{ E }[/math] in [math]\displaystyle{ \Sigma, }[/math] we have [math]\displaystyle{ \mu(E) \geq 0. }[/math]
  • Null empty set: [math]\displaystyle{ \mu(\varnothing) = 0. }[/math]
  • Countable additivity (or [math]\displaystyle{ \sigma }[/math]-additivity): For all countable collections [math]\displaystyle{ \{ E_k \}_{k=1}^\infty }[/math] of pairwise disjoint sets in Σ,[math]\displaystyle{ \mu\left(\bigcup_{k=1}^\infty E_k\right)=\sum_{k=1}^\infty \mu(E_k). }[/math]

If at least one set [math]\displaystyle{ E }[/math] has finite measure, then the requirement that [math]\displaystyle{ \mu(\varnothing) = 0 }[/math] is met automatically. Indeed, by countable additivity, [math]\displaystyle{ \mu(E)=\mu(E \cup \varnothing) = \mu(E) + \mu(\varnothing), }[/math] and therefore [math]\displaystyle{ \mu(\varnothing)=0. }[/math]

If the condition of non-negativity is omitted but the second and third of these conditions are met, and [math]\displaystyle{ \mu }[/math] takes on at most one of the values [math]\displaystyle{ \pm \infty, }[/math] then [math]\displaystyle{ \mu }[/math] is called a signed measure.

The pair [math]\displaystyle{ (X, \Sigma) }[/math] is called a measurable space, the members of [math]\displaystyle{ \Sigma }[/math] are called measurable sets.

A triple [math]\displaystyle{ (X, \Sigma, \mu) }[/math] is called a measure space. A probability measure is a measure with total measure one – that is, [math]\displaystyle{ \mu(X) = 1. }[/math] A probability space is a measure space with a probability measure.

For measure spaces that are also topological spaces various compatibility conditions can be placed for the measure and the topology. Most measures met in practice in analysis (and in many cases also in probability theory) are Radon measures. Radon measures have an alternative definition in terms of linear functionals on the locally convex topological vector space of continuous functions with compact support. This approach is taken by Bourbaki (2004) and a number of other sources. For more details, see the article on Radon measures.

Instances

Some important measures are listed here.

  • The counting measure is defined by [math]\displaystyle{ \mu(S) }[/math] = number of elements in [math]\displaystyle{ S. }[/math]
  • The Lebesgue measure on [math]\displaystyle{ \R }[/math] is a complete translation-invariant measure on a σ-algebra containing the intervals in [math]\displaystyle{ \R }[/math] such that [math]\displaystyle{ \mu([0, 1]) = 1 }[/math]; and every other measure with these properties extends Lebesgue measure.
  • Circular angle measure is invariant under rotation, and hyperbolic angle measure is invariant under squeeze mapping.
  • The Haar measure for a locally compact topological group is a generalization of the Lebesgue measure (and also of counting measure and circular angle measure) and has similar uniqueness properties.
  • The Hausdorff measure is a generalization of the Lebesgue measure to sets with non-integer dimension, in particular, fractal sets.
  • Every probability space gives rise to a measure which takes the value 1 on the whole space (and therefore takes all its values in the unit interval [0, 1]). Such a measure is called a probability measure. See probability axioms.
  • The Dirac measure δa (cf. Dirac delta function) is given by δa(S) = χS(a), where χS is the indicator function of [math]\displaystyle{ S. }[/math] The measure of a set is 1 if it contains the point [math]\displaystyle{ a }[/math] and 0 otherwise.

Other 'named' measures used in various theories include: Borel measure, Jordan measure, ergodic measure, Gaussian measure, Baire measure, Radon measure, Young measure, and Loeb measure.

In physics an example of a measure is spatial distribution of mass (see for example, gravity potential), or another non-negative extensive property, conserved (see conservation law for a list of these) or not. Negative values lead to signed measures, see "generalizations" below.

  • Liouville measure, known also as the natural volume form on a symplectic manifold, is useful in classical statistical and Hamiltonian mechanics.
  • Gibbs measure is widely used in statistical mechanics, often under the name canonical ensemble.

Basic properties

Let [math]\displaystyle{ \mu }[/math] be a measure.

Monotonicity

If [math]\displaystyle{ E_1 }[/math] and [math]\displaystyle{ E_2 }[/math] are measurable sets with [math]\displaystyle{ E_1 \subseteq E_2 }[/math] then [math]\displaystyle{ \mu(E_1) \leq \mu(E_2). }[/math]

Measure of countable unions and intersections

Subadditivity

For any countable sequence [math]\displaystyle{ E_1, E_2, E_3, \ldots }[/math] of (not necessarily disjoint) measurable sets [math]\displaystyle{ E_n }[/math] in [math]\displaystyle{ \Sigma: }[/math] [math]\displaystyle{ \mu\left( \bigcup_{i=1}^\infty E_i\right) \leq \sum_{i=1}^\infty \mu(E_i). }[/math]

Continuity from below

If [math]\displaystyle{ E_1, E_2, E_3, \ldots }[/math] are measurable sets that are increasing (meaning that [math]\displaystyle{ E_1 \subseteq E_2 \subseteq E_3 \subseteq \ldots }[/math]) then the union of the sets [math]\displaystyle{ E_n }[/math] is measurable and [math]\displaystyle{ \mu\left(\bigcup_{i=1}^\infty E_i\right) ~=~ \lim_{i\to\infty} \mu(E_i) = \sup_{i \geq 1} \mu(E_i). }[/math]

Continuity from above

If [math]\displaystyle{ E_1, E_2, E_3, \ldots }[/math] are measurable sets that are decreasing (meaning that [math]\displaystyle{ E_1 \supseteq E_2 \supseteq E_3 \supseteq \ldots }[/math]) then the intersection of the sets [math]\displaystyle{ E_n }[/math] is measurable; furthermore, if at least one of the [math]\displaystyle{ E_n }[/math] has finite measure then [math]\displaystyle{ \mu\left(\bigcap_{i=1}^\infty E_i\right) = \lim_{i\to\infty} \mu(E_i) = \inf_{i \geq 1} \mu(E_i). }[/math]

This property is false without the assumption that at least one of the [math]\displaystyle{ E_n }[/math] has finite measure. For instance, for each [math]\displaystyle{ n \in \N, }[/math] let [math]\displaystyle{ E_n = [n, \infty) \subseteq \R, }[/math] which all have infinite Lebesgue measure, but the intersection is empty.

Other properties

Completeness

Main page: Complete measure

A measurable set [math]\displaystyle{ X }[/math] is called a null set if [math]\displaystyle{ \mu(X) = 0. }[/math] A subset of a null set is called a negligible set. A negligible set need not be measurable, but every measurable negligible set is automatically a null set. A measure is called complete if every negligible set is measurable.

A measure can be extended to a complete one by considering the σ-algebra of subsets [math]\displaystyle{ Y }[/math] which differ by a negligible set from a measurable set [math]\displaystyle{ X, }[/math] that is, such that the symmetric difference of [math]\displaystyle{ X }[/math] and [math]\displaystyle{ Y }[/math] is contained in a null set. One defines [math]\displaystyle{ \mu(Y) }[/math] to equal [math]\displaystyle{ \mu(X). }[/math]

μ{x : f(x) ≥ t} = μ{x : f(x) > t} (a.e.)

If [math]\displaystyle{ f:X\to[0,+\infty] }[/math] is [math]\displaystyle{ (\Sigma,{\cal B}([0,+\infty])) }[/math]-measurable, then [math]\displaystyle{ \mu\{x\in X: f(x) \geq t\} = \mu\{x\in X: f(x) \gt t\} }[/math] for almost all [math]\displaystyle{ t \in X. }[/math][1] This property is used in connection with Lebesgue integral.

Additivity

Measures are required to be countably additive. However, the condition can be strengthened as follows. For any set [math]\displaystyle{ I }[/math] and any set of nonnegative [math]\displaystyle{ r_i,i\in I }[/math] define: [math]\displaystyle{ \sum_{i\in I} r_i=\sup\left\lbrace\sum_{i\in J} r_i : |J|\lt \aleph_0, J\subseteq I\right\rbrace. }[/math] That is, we define the sum of the [math]\displaystyle{ r_i }[/math] to be the supremum of all the sums of finitely many of them.

A measure [math]\displaystyle{ \mu }[/math] on [math]\displaystyle{ \Sigma }[/math] is [math]\displaystyle{ \kappa }[/math]-additive if for any [math]\displaystyle{ \lambda\lt \kappa }[/math] and any family of disjoint sets [math]\displaystyle{ X_\alpha,\alpha\lt \lambda }[/math] the following hold: [math]\displaystyle{ \bigcup_{\alpha\in\lambda} X_\alpha \in \Sigma }[/math] [math]\displaystyle{ \mu\left(\bigcup_{\alpha\in\lambda} X_\alpha\right) = \sum_{\alpha\in\lambda}\mu\left(X_\alpha\right). }[/math] Note that the second condition is equivalent to the statement that the ideal of null sets is [math]\displaystyle{ \kappa }[/math]-complete.

Sigma-finite measures

A measure space [math]\displaystyle{ (X, \Sigma, \mu) }[/math] is called finite if [math]\displaystyle{ \mu(X) }[/math] is a finite real number (rather than [math]\displaystyle{ \infty }[/math]). Nonzero finite measures are analogous to probability measures in the sense that any finite measure [math]\displaystyle{ \mu }[/math] is proportional to the probability measure [math]\displaystyle{ \frac{1}{\mu(X)}\mu. }[/math] A measure [math]\displaystyle{ \mu }[/math] is called σ-finite if [math]\displaystyle{ X }[/math] can be decomposed into a countable union of measurable sets of finite measure. Analogously, a set in a measure space is said to have a σ-finite measure if it is a countable union of sets with finite measure.

For example, the real numbers with the standard Lebesgue measure are σ-finite but not finite. Consider the closed intervals [math]\displaystyle{ [k, k+1] }[/math] for all integers [math]\displaystyle{ k; }[/math] there are countably many such intervals, each has measure 1, and their union is the entire real line. Alternatively, consider the real numbers with the counting measure, which assigns to each finite set of reals the number of points in the set. This measure space is not σ-finite, because every set with finite measure contains only finitely many points, and it would take uncountably many such sets to cover the entire real line. The σ-finite measure spaces have some very convenient properties; σ-finiteness can be compared in this respect to the Lindelöf property of topological spaces.Template:OR inline They can be also thought of as a vague generalization of the idea that a measure space may have 'uncountable measure'.

Strictly localizable measures

Main page: Decomposable measure

Semifinite measures

Let [math]\displaystyle{ X }[/math] be a set, let [math]\displaystyle{ {\cal A} }[/math] be a sigma-algebra on [math]\displaystyle{ X, }[/math] and let [math]\displaystyle{ \mu }[/math] be a measure on [math]\displaystyle{ {\cal A}. }[/math] We say [math]\displaystyle{ \mu }[/math] is semifinite to mean that for all [math]\displaystyle{ A\in\mu^\text{pre}\{+\infty\}, }[/math] [math]\displaystyle{ {\cal P}(A)\cap\mu^\text{pre}(\R_{\gt 0})\ne\emptyset. }[/math][2]

Semifinite measures generalize sigma-finite measures, in such a way that some big theorems of measure theory that hold for sigma-finite but not arbitrary measures can be extended with little modification to hold for semifinite measures. (To-do: add examples of such theorems; cf. the talk page.)

Basic examples

  • Every sigma-finite measure is semifinite.
  • Assume [math]\displaystyle{ {\cal A}={\cal P}(X), }[/math] let [math]\displaystyle{ f:X\to[0,+\infty], }[/math] and assume [math]\displaystyle{ \mu(A)=\sum_{a\in A}f(a) }[/math] for all [math]\displaystyle{ A\subseteq X. }[/math]
    • We have that [math]\displaystyle{ \mu }[/math] is sigma-finite if and only if [math]\displaystyle{ f(x)\lt +\infty }[/math] for all [math]\displaystyle{ x\in X }[/math] and [math]\displaystyle{ f^\text{pre}(\R_{\gt 0}) }[/math] is countable. We have that [math]\displaystyle{ \mu }[/math] is semifinite if and only if [math]\displaystyle{ f(x)\lt +\infty }[/math] for all [math]\displaystyle{ x\in X. }[/math][3]
    • Taking [math]\displaystyle{ f=X\times\{1\} }[/math] above (so that [math]\displaystyle{ \mu }[/math] is counting measure on [math]\displaystyle{ {\cal P}(X) }[/math]), we see that counting measure on [math]\displaystyle{ {\cal P}(X) }[/math] is
      • sigma-finite if and only if [math]\displaystyle{ X }[/math] is countable; and
      • semifinite (without regard to whether [math]\displaystyle{ X }[/math] is countable). (Thus, counting measure, on the power set [math]\displaystyle{ {\cal P}(X) }[/math] of an arbitrary uncountable set [math]\displaystyle{ X, }[/math] gives an example of a semifinite measure that is not sigma-finite.)
  • Let [math]\displaystyle{ d }[/math] be a complete, separable metric on [math]\displaystyle{ X, }[/math] let [math]\displaystyle{ {\cal B} }[/math] be the Borel sigma-algebra induced by [math]\displaystyle{ d, }[/math] and let [math]\displaystyle{ s\in\R_{\gt 0}. }[/math] Then the Hausdorff measure [math]\displaystyle{ {\cal H}^s|{\cal B} }[/math] is semifinite.[4]
  • Let [math]\displaystyle{ d }[/math] be a complete, separable metric on [math]\displaystyle{ X, }[/math] let [math]\displaystyle{ {\cal B} }[/math] be the Borel sigma-algebra induced by [math]\displaystyle{ d, }[/math] and let [math]\displaystyle{ s\in\R_{\gt 0}. }[/math] Then the packing measure [math]\displaystyle{ {\cal H}^s|{\cal B} }[/math] is semifinite.[5]

Involved example

The zero measure is sigma-finite and thus semifinite. In addition, the zero measure is clearly less than or equal to [math]\displaystyle{ \mu. }[/math] It can be shown there is a greatest measure with these two properties:

Theorem (semifinite part)[6] — For any measure [math]\displaystyle{ \mu }[/math] on [math]\displaystyle{ {\cal A}, }[/math] there exists, among semifinite measures on [math]\displaystyle{ {\cal A} }[/math] that are less than or equal to [math]\displaystyle{ \mu, }[/math] a greatest element [math]\displaystyle{ \mu_\text{sf}. }[/math]

We say the semifinite part of [math]\displaystyle{ \mu }[/math] to mean the semifinite measure [math]\displaystyle{ \mu_\text{sf} }[/math] defined in the above theorem. We give some nice, explicit formulas, which some authors may take as definition, for the semifinite part:

  • [math]\displaystyle{ \mu_\text{sf}=(\sup\{\mu(B):B\in{\cal P}(A)\cap\mu^\text{pre}(\R_{\ge0})\})_{A\in{\cal A}}. }[/math][6]
  • [math]\displaystyle{ \mu_\text{sf}=(\sup\{\mu(A\cap B):B\in\mu^\text{pre}(\R_{\ge0})\})_{A\in{\cal A}}\}. }[/math][7]
  • [math]\displaystyle{ \mu_\text{sf}=\mu|_{\mu^\text{pre}(\R_{\gt 0})}\cup\{A\in{\cal A}:\sup\{\mu(B):B\in{\cal P}(A)\}=+\infty\}\times\{+\infty\}\cup\{A\in{\cal A}:\sup\{\mu(B):B\in{\cal P}(A)\}\lt +\infty\}\times\{0\}. }[/math][8]

Since [math]\displaystyle{ \mu_\text{sf} }[/math] is semifinite, it follows that if [math]\displaystyle{ \mu=\mu_\text{sf} }[/math] then [math]\displaystyle{ \mu }[/math] is semifinite. It is also evident that if [math]\displaystyle{ \mu }[/math] is semifinite then [math]\displaystyle{ \mu=\mu_\text{sf}. }[/math]

Non-examples

Every [math]\displaystyle{ 0-\infty }[/math] measure that is not the zero measure is not semifinite. (Here, we say [math]\displaystyle{ 0-\infty }[/math] measure to mean a measure whose range lies in [math]\displaystyle{ \{0,+\infty\} }[/math]: [math]\displaystyle{ (\forall A\in{\cal A})(\mu(A)\in\{0,+\infty\}). }[/math]) Below we give examples of [math]\displaystyle{ 0-\infty }[/math] measures that are not zero measures.

  • Let [math]\displaystyle{ X }[/math] be nonempty, let [math]\displaystyle{ {\cal A} }[/math] be a [math]\displaystyle{ \sigma }[/math]-algebra on [math]\displaystyle{ X, }[/math] let [math]\displaystyle{ f:X\to\{0,+\infty\} }[/math] be not the zero function, and let [math]\displaystyle{ \mu=(\sum_{x\in A}f(x))_{A\in{\cal A}}. }[/math] It can be shown that [math]\displaystyle{ \mu }[/math] is a measure.
    • [math]\displaystyle{ \mu=\{(\emptyset,0)\}\cup({\cal A}\setminus\{\emptyset\})\times\{+\infty\}. }[/math][9]
      • [math]\displaystyle{ X=\{0\}, }[/math] [math]\displaystyle{ {\cal A}=\{\emptyset,X\}, }[/math] [math]\displaystyle{ \mu=\{(\emptyset,0),(X,+\infty)\}. }[/math][10]
  • Let [math]\displaystyle{ X }[/math] be uncountable, let [math]\displaystyle{ {\cal A} }[/math] be a [math]\displaystyle{ \sigma }[/math]-algebra on [math]\displaystyle{ X, }[/math] let [math]\displaystyle{ {\cal C}=\{A\in{\cal A}:A\text{ is countable}\} }[/math] be the countable elements of [math]\displaystyle{ {\cal A}, }[/math] and let [math]\displaystyle{ \mu={\cal C}\times\{0\}\cup({\cal A}\setminus{\cal C})\times\{+\infty\}. }[/math] It can be shown that [math]\displaystyle{ \mu }[/math] is a measure.[2]

Involved non-example

Measures that are not semifinite are very wild when restricted to certain sets.[Note 1] Every measure is, in a sense, semifinite once its [math]\displaystyle{ 0-\infty }[/math] part (the wild part) is taken away.

Theorem (Luther decomposition)[11][12] — For any measure [math]\displaystyle{ \mu }[/math] on [math]\displaystyle{ {\cal A}, }[/math] there exists a [math]\displaystyle{ 0-\infty }[/math] measure [math]\displaystyle{ \xi }[/math] on [math]\displaystyle{ {\cal A} }[/math] such that [math]\displaystyle{ \mu=\nu+\xi }[/math] for some semifinite measure [math]\displaystyle{ \nu }[/math] on [math]\displaystyle{ {\cal A}. }[/math] In fact, among such measures [math]\displaystyle{ \xi, }[/math] there exists a least measure [math]\displaystyle{ \mu_{0-\infty}. }[/math] Also, we have [math]\displaystyle{ \mu=\mu_\text{sf}+\mu_{0-\infty}. }[/math]

We say the [math]\displaystyle{ \mathbf{0-\infty} }[/math] part of [math]\displaystyle{ \mu }[/math] to mean the measure [math]\displaystyle{ \mu_{0-\infty} }[/math] defined in the above theorem. Here is an explicit formula for [math]\displaystyle{ \mu_{0-\infty} }[/math]: [math]\displaystyle{ \mu_{0-\infty}=(\sup\{\mu(B)-\mu_\text{sf}(B):B\in{\cal P}(A)\cap\mu_\text{sf}^\text{pre}(\R_{\ge0})\})_{A\in{\cal A}}. }[/math]

Results regarding semifinite measures

  • Let [math]\displaystyle{ \mathbb F }[/math] be [math]\displaystyle{ \R }[/math] or [math]\displaystyle{ \C, }[/math] and let [math]\displaystyle{ T:L_\mathbb{F}^\infty(\mu)\to\left(L_\mathbb{F}^1(\mu)\right)^*:g\mapsto T_g=\left(\int fgd\mu\right)_{f\in L_\mathbb{F}^1(\mu)}. }[/math] Then [math]\displaystyle{ \mu }[/math] is semifinite if and only if [math]\displaystyle{ T }[/math] is injective.[13][14] (This result has import in the study of the dual space of [math]\displaystyle{ L^1=L \mathbb{F}^1(\mu) }[/math].)
  • Let [math]\displaystyle{ \mathbb F }[/math] be [math]\displaystyle{ \R }[/math] or [math]\displaystyle{ \C, }[/math] and let [math]\displaystyle{ {\cal T} }[/math] be the topology of convergence in measure on [math]\displaystyle{ L_\mathbb{F}^0(\mu). }[/math] Then [math]\displaystyle{ \mu }[/math] is semifinite if and only if [math]\displaystyle{ {\cal T} }[/math] is Hausdorff.[15][16]
  • (Johnson) Let [math]\displaystyle{ X }[/math] be a set, let [math]\displaystyle{ {\cal A} }[/math] be a sigma-algebra on [math]\displaystyle{ X, }[/math] let [math]\displaystyle{ \mu }[/math] be a measure on [math]\displaystyle{ {\cal A}, }[/math] let [math]\displaystyle{ Y }[/math] be a set, let [math]\displaystyle{ {\cal B} }[/math] be a sigma-algebra on [math]\displaystyle{ Y, }[/math] and let [math]\displaystyle{ \nu }[/math] be a measure on [math]\displaystyle{ {\cal B}. }[/math] If [math]\displaystyle{ \mu,\nu }[/math] are both not a [math]\displaystyle{ 0-\infty }[/math] measure, then both [math]\displaystyle{ \mu }[/math] and [math]\displaystyle{ \nu }[/math] are semifinite if and only if [math]\displaystyle{ (\mu\times \text{cld}\nu) }[/math][math]\displaystyle{ (A\times B)=\mu(A)\nu(B) }[/math] for all [math]\displaystyle{ A\in{\cal A} }[/math] and [math]\displaystyle{ B\in{\cal B}. }[/math] (Here, [math]\displaystyle{ \mu\times_\text{cld}\nu }[/math] is the measure defined in Theorem 39.1 in Berberian '65.[17])

Localizable measures

Localizable measures are a special case of semifinite measures and a generalization of sigma-finite measures.

Let [math]\displaystyle{ X }[/math] be a set, let [math]\displaystyle{ {\cal A} }[/math] be a sigma-algebra on [math]\displaystyle{ X, }[/math] and let [math]\displaystyle{ \mu }[/math] be a measure on [math]\displaystyle{ {\cal A}. }[/math]

  • Let [math]\displaystyle{ \mathbb F }[/math] be [math]\displaystyle{ \R }[/math] or [math]\displaystyle{ \C, }[/math] and let [math]\displaystyle{ T : L_\mathbb{F}^\infty(\mu) \to \left(L_\mathbb{F}^1(\mu)\right)^* : g \mapsto T_g = \left(\int fgd\mu\right)_{f\in L_\mathbb{F}^1(\mu)}. }[/math] Then [math]\displaystyle{ \mu }[/math] is localizable if and only if [math]\displaystyle{ T }[/math] is bijective (if and only if [math]\displaystyle{ L_\mathbb{F}^\infty(\mu) }[/math] "is" [math]\displaystyle{ L_\mathbb{F}^1(\mu)^* }[/math]).[18][14]

s-finite measures

Main page: S-finite measure

A measure is said to be s-finite if it is a countable sum of bounded measures. S-finite measures are more general than sigma-finite ones and have applications in the theory of stochastic processes.

Non-measurable sets

Main page: Non-measurable set

If the axiom of choice is assumed to be true, it can be proved that not all subsets of Euclidean space are Lebesgue measurable; examples of such sets include the Vitali set, and the non-measurable sets postulated by the Hausdorff paradox and the Banach–Tarski paradox.

Generalizations

For certain purposes, it is useful to have a "measure" whose values are not restricted to the non-negative reals or infinity. For instance, a countably additive set function with values in the (signed) real numbers is called a signed measure, while such a function with values in the complex numbers is called a complex measure. Observe, however, that complex measure is necessarily of finite variation, hence complex measures include finite signed measures but not, for example, the Lebesgue measure.

Measures that take values in Banach spaces have been studied extensively.[19] A measure that takes values in the set of self-adjoint projections on a Hilbert space is called a projection-valued measure; these are used in functional analysis for the spectral theorem. When it is necessary to distinguish the usual measures which take non-negative values from generalizations, the term positive measure is used. Positive measures are closed under conical combination but not general linear combination, while signed measures are the linear closure of positive measures.

Another generalization is the finitely additive measure, also known as a content. This is the same as a measure except that instead of requiring countable additivity we require only finite additivity. Historically, this definition was used first. It turns out that in general, finitely additive measures are connected with notions such as Banach limits, the dual of [math]\displaystyle{ L^\infty }[/math] and the Stone–Čech compactification. All these are linked in one way or another to the axiom of choice. Contents remain useful in certain technical problems in geometric measure theory; this is the theory of Banach measures.

A charge is a generalization in both directions: it is a finitely additive, signed measure.[20] (Cf. ba space for information about bounded charges, where we say a charge is bounded to mean its range its a bounded subset of R.)

See also


Notes

  1. One way to rephrase our definition is that [math]\displaystyle{ \mu }[/math] is semifinite if and only if [math]\displaystyle{ (\forall A\in\mu^\text{pre}\{+\infty\})(\exists B\subseteq A)(0\lt \mu(B)\lt +\infty). }[/math] Negating this rephrasing, we find that [math]\displaystyle{ \mu }[/math] is not semifinite if and only if [math]\displaystyle{ (\exists A\in\mu^\text{pre}\{+\infty\})(\forall B\subseteq A)(\mu(B)\in\{0,+\infty\}). }[/math] For every such set [math]\displaystyle{ A, }[/math] the subspace measure induced by the subspace sigma-algebra induced by [math]\displaystyle{ A, }[/math] i.e. the restriction of [math]\displaystyle{ \mu }[/math] to said subspace sigma-algebra, is a [math]\displaystyle{ 0-\infty }[/math] measure that is not the zero measure.

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  • M. E. Munroe, 1953. Introduction to Measure and Integration. Addison Wesley.
  • Nielsen, Ole A (1997). An Introduction to Integration and Measure Theory. Wiley. ISBN 0-471-59518-7. 
  • K. P. S. Bhaskara Rao and M. Bhaskara Rao (1983), Theory of Charges: A Study of Finitely Additive Measures, London: Academic Press, pp. x + 315, ISBN 0-12-095780-9 
  • Royden, H.L.; Fitzpatrick, P.M. (2010). Real Analysis (Fourth ed.). Prentice Hall. p. 342, Exercise 17.8.  First printing. Note that there is a later (2017) second printing. Though usually there is little difference between the first and subsequent printings, in this case the second printing not only deletes from page 53 the Exercises 36, 40, 41, and 42 of Chapter 2 but also offers a (slightly, but still substantially) different presentation of part (ii) of Exercise 17.8. (The second printing's presentation of part (ii) of Exercise 17.8 (on the Luther[11] decomposition) agrees with usual presentations,[2][21] whereas the first printing's presentation provides a fresh perspective.)
  • Shilov, G. E., and Gurevich, B. L., 1978. Integral, Measure, and Derivative: A Unified Approach, Richard A. Silverman, trans. Dover Publications. ISBN 0-486-63519-8. Emphasizes the Daniell integral.
  • Teschl, Gerald, Topics in Real and Functional Analysis, (lecture notes), https://www.mat.univie.ac.at/~gerald/ftp/book-fa/index.html 
  • Tao, Terence (2011). An Introduction to Measure Theory. Providence, R.I.: American Mathematical Society. ISBN 9780821869192. 
  • Weaver, Nik (2013). Measure Theory and Functional Analysis. World Scientific. ISBN 9789814508568. 

References

  1. Fremlin, D. H. (2010), Measure Theory, 2 (Second ed.), p. 221 
  2. 2.0 2.1 2.2 Mukherjea 1985, p. 90.
  3. Folland 1999, p. 25.
  4. Edgar 1998, Theorem 1.5.2, p. 42.
  5. Edgar 1998, Theorem 1.5.3, p. 42.
  6. 6.0 6.1 Nielsen 1997, Exercise 11.30, p. 159.
  7. Fremlin 2016, Section 213X, part (c).
  8. Royden 2010, Exercise 17.8, p. 342.
  9. Hewitt 1965, part (b) of Example 10.4, p. 127.
  10. Fremlin 2016, Section 211O, p. 15.
  11. 11.0 11.1 Luther 1967, Theorem 1.
  12. Mukherjea 1985, part (b) of Proposition 2.3, p. 90.
  13. Fremlin 2016, part (a) of Theorem 243G, p. 159.
  14. 14.0 14.1 Fremlin 2016, Section 243K, p. 162.
  15. Fremlin 2016, part (a) of the Theorem in Section 245E, p. 182.
  16. Fremlin 2016, Section 245M, p. 188.
  17. Berberian 1965, Theorem 39.1, p. 129.
  18. Fremlin 2016, part (b) of Theorem 243G, p. 159.
  19. Rao, M. M. (2012), Random and Vector Measures, Series on Multivariate Analysis, 9, World Scientific, ISBN 978-981-4350-81-5 .
  20. Bhaskara Rao, K. P. S. (1983). Theory of charges: a study of finitely additive measures. M. Bhaskara Rao. London: Academic Press. pp. 35. ISBN 0-12-095780-9. OCLC 21196971. https://www.worldcat.org/oclc/21196971. 
  21. Folland 1999, p. 27, Exercise 1.15.a.

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