Katana VentraIP

Measure (mathematics)

In mathematics, the concept of a measure is a generalization and formalization of geometrical measures (length, area, volume) and other common notions, such as magnitude, 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.

For the coalgebraic concept, see Measuring coalgebra.

The intuition behind this concept dates back to ancient Greece, when Archimedes tried to calculate the area of a circle.[1] 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.

Non-negativity: For all

Countable additivity (or ): For all countable collections of pairwise disjoint sets in Σ,

-additivity

Let be a set and a -algebra over A set function from to the extended real number line is called a measure if the following conditions hold:


If at least one set has finite measure, then the requirement is met automatically due to countable additivity:


If the condition of non-negativity is dropped, and takes on at most one of the values of then is called a signed measure.


The pair is called a measurable space, and the members of are called measurable sets.


A triple is called a measure space. A probability measure is a measure with total measure one – that is, 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.

The is defined by = number of elements in

counting measure

The on is a complete translation-invariant measure on a σ-algebra containing the intervals in such that ; and every other measure with these properties extends the Lebesgue measure.

Lebesgue measure

Circular measure is invariant under rotation, and hyperbolic angle measure is invariant under squeeze mapping.

angle

The 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.

Haar measure

The is a generalization of the Lebesgue measure to sets with non-integer dimension, in particular, fractal sets.

Hausdorff measure

Every 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 or distribution. See the list of probability distributions for instances.

probability space

The δa (cf. Dirac delta function) is given by δa(S) = χS(a), where χS is the indicator function of The measure of a set is 1 if it contains the point and 0 otherwise.

Dirac measure

Some important measures are listed here.


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.


Measure theory is used in machine learning. One example is the Flow Induced Probability Measure in GFlowNet.[2]

Every sigma-finite measure is semifinite.

[5]

Let be a complete, separable metric on let be the Borel sigma-algebra induced by and let Then the is semifinite.[6]

Hausdorff measure

Let be a complete, separable metric on let be the Borel sigma-algebra induced by and let Then the is semifinite.[7]

packing measure

Generalizations[edit]

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.[21] 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 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.[22] (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.)

, Encyclopedia of Mathematics, EMS Press, 2001 [1994]

"Measure"

Tutorial: Measure Theory for Dummies