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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.

- Definition
- Instances
- Basic properties
- Monotonicity
- Measure of countable unions and intersections
- Other properties
- Completeness
- μ{x : f(x) ≥ t} = μ{x : f(x) > t} (a.e.)
- Additivity
- Sigma-finite measures
- Strictly localizable measures
- Semifinite measures
- Localizable measures
- s-finite measures
- Non-measurable sets
- Generalizations
- See also
- Notes
- Bibliography
- References
- External links

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.

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:

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

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

and therefore

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.

Some important measures are listed here.

- The counting measure is defined by = number of elements in
- The Lebesgue measure 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 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*or*distribution*. See the list of probability distributions for instances. - The Dirac measure
*δ*_{a}(cf. Dirac delta function) is given by*δ*_{a}(*S*) =*χ*_{S}(a), where*χ*_{S}is the indicator function of The measure of a set is 1 if it contains the point 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.

Let be a measure.

If and are measurable sets with then

For any countable sequence of (not necessarily disjoint) measurable sets in

If are measurable sets that are increasing (meaning that ) then the union of the sets is measurable and

If are measurable sets that are decreasing (meaning that ) then the intersection of the sets is measurable; furthermore, if at least one of the has finite measure then

This property is false without the assumption that at least one of the has finite measure. For instance, for each let which all have infinite Lebesgue measure, but the intersection is empty.

A measurable set is called a * null set * if 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 which differ by a negligible set from a measurable set that is, such that the symmetric difference of and is contained in a null set. One defines to equal

If is -measurable, then

for almost all ^{ [1] } This property is used in connection with Lebesgue integral.

Both and are monotonically non-increasing functions of so both of them have at most countably many discontinuities and thus they are continuous almost everywhere, relative to the Lebesgue measure. If then so that as desired.

If is such that then monotonicity implies

so that as required. If for all then we are done, so assume otherwise. Then there is a unique such that is infinite to the left of (which can only happen when ) and finite to the right. Arguing as above, when Similarly, if and then

For let be a monotonically non-decreasing sequence converging to The monotonically non-increasing sequence of members of has at least one finitely -measurable component, and

Continuity from above guarantees that

The right-hand side then equals if is a point of continuity of Since is continuous almost everywhere, this completes the proof.

Measures are required to be countably additive. However, the condition can be strengthened as follows. For any set and any set of nonnegative define:

That is, we define the sum of the to be the supremum of all the sums of finitely many of them.

A measure on is -additive if for any and any family of disjoint sets the following hold:

The second condition is equivalent to the statement that the ideal of null sets is -complete.

A measure space is called finite if is a finite real number (rather than ). Nonzero finite measures are analogous to probability measures in the sense that any finite measure is proportional to the probability measure A measure is called *σ-finite* if 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 for all integers 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.^{[ original research? ]} They can be also thought of as a vague generalization of the idea that a measure space may have 'uncountable measure'.

Let be a set, let be a sigma-algebra on and let be a measure on We say is **semifinite** to mean that for all ^{ [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.)

- Every sigma-finite measure is semifinite.
- Assume let and assume for all
- We have that is sigma-finite if and only if for all and is countable. We have that is semifinite if and only if for all
^{ [3] } - Taking above (so that is counting measure on ), we see that counting measure on is
- sigma-finite if and only if is countable; and
- semifinite (without regard to whether is countable). (Thus, counting measure, on the power set of an arbitrary uncountable set gives an example of a semifinite measure that is not sigma-finite.)

- We have that is sigma-finite if and only if for all and is countable. We have that is semifinite if and only if for all
- Let be a complete, separable metric on let be the Borel sigma-algebra induced by and let Then the Hausdorff measure is semifinite.
^{ [4] } - Let be a complete, separable metric on let be the Borel sigma-algebra induced by and let Then the packing measure is semifinite.
^{ [5] }

The zero measure is sigma-finite and thus semifinite. In addition, the zero measure is clearly less than or equal to It can be shown there is a greatest measure with these two properties:

**Theorem (semifinite part) ^{ [6] }** — For any measure on there exists, among semifinite measures on that are less than or equal to a greatest element

We say the **semifinite part** of to mean the semifinite measure defined in the above theorem. We give some nice, explicit formulas, which some authors may take as definition, for the semifinite part:

^{ [6] }^{ [7] }^{ [8] }

Since is semifinite, it follows that if then is semifinite. It is also evident that if is semifinite then

Every * measure* that is not the zero measure is not semifinite. (Here, we say * measure* to mean a measure whose range lies in : ) Below we give examples of measures that are not zero measures.

- Let be nonempty, let be a -algebra on let be not the zero function, and let It can be shown that is a measure.
^{ [9] }^{ [10] }

- Let be uncountable, let be a -algebra on let be the countable elements of and let It can be shown that is a measure.
^{ [2] }

Measures that are not semifinite are very wild when restricted to certain sets.

^{ [Note 1] }Every measure is, in a sense, semifinite once its part (the wild part) is taken away.— A. Mukherjea and K. Pothoven,Real and Functional Analysis, Part A: Real Analysis(1985)

**Theorem (Luther decomposition) ^{ [11] }^{ [12] }** — For any measure on there exists a measure on such that for some semifinite measure on In fact, among such measures there exists a least measure Also, we have

We say the ** part** of to mean the measure defined in the above theorem. Here is an explicit formula for :

- Let be or and let Then is semifinite if and only if is injective.
^{ [13] }^{ [14] }(This result has import in the study of the dual space of .) - Let be or and let be the topology of convergence in measure on Then is semifinite if and only if is Hausdorff.
^{ [15] }^{ [16] } - (Johnson) Let be a set, let be a sigma-algebra on let be a measure on let be a set, let be a sigma-algebra on and let be a measure on If are both not a measure, then both and are semifinite if and only if for all and (Here, is the measure defined in Theorem 39.1 in Berberian '65.
^{ [17] })

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

Let be a set, let be a sigma-algebra on and let be a measure on

- Let be or and let Then is localizable if and only if is bijective (if and only if "is" ).
^{ [18] }^{ [14] }

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.

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.

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 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*.)

- Abelian von Neumann algebra
- Almost everywhere
- Carathéodory's extension theorem
- Content (measure theory)
- Fubini's theorem
- Fatou's lemma
- Fuzzy measure theory
- Geometric measure theory
- Hausdorff measure
- Inner measure
- Lebesgue integration
- Lebesgue measure
- Lorentz space
- Lifting theory
- Measurable cardinal
- Measurable function
- Minkowski content
- Outer measure
- Product measure
- Pushforward measure
- Regular measure
- Vector measure
- Valuation (measure theory)
- Volume form

- ↑ One way to rephrase our definition is that is semifinite if and only if Negating this rephrasing, we find that is not semifinite if and only if For every such set the subspace measure induced by the subspace sigma-algebra induced by i.e. the restriction of to said subspace sigma-algebra, is a measure that is not the zero measure.

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*Measure and Integration Theory*, Berlin: de Gruyter, ISBN 978-3110167191 - Bear, H.S. (2001),
*A Primer of Lebesgue Integration*, San Diego: Academic Press, ISBN 978-0120839711 - Berberian, Sterling K (1965).
*Measure and Integration*. MacMillan. - Bogachev, V. I. (2006),
*Measure theory*, Berlin: Springer, ISBN 978-3540345138 - Bourbaki, Nicolas (2004),
*Integration I*, Springer Verlag, ISBN 3-540-41129-1 Chapter III. - R. M. Dudley, 2002.
*Real Analysis and Probability*. Cambridge University Press. - Edgar, Gerald A (1998).
*Integral, Probability, and Fractal Measures*. Springer. ISBN 978-1-4419-3112-2. - Folland, Gerald B (1999).
*Real Analysis: Modern Techniques and Their Applications*(Second ed.). Wiley. ISBN 0-471-31716-0. - Federer, Herbert. Geometric measure theory. Die Grundlehren der mathematischen Wissenschaften, Band 153 Springer-Verlag New York Inc., New York 1969 xiv+676 pp.
- Fremlin, D.H. (2016).
*Measure Theory, Volume 2: Broad Foundations*(Hardback ed.). Torres Fremlin. Second printing. - Hewitt, Edward; Stromberg, Karl (1965).
*Real and Abstract Analysis: A Modern Treatment of the Theory of Functions of a Real Variable*. Springer. ISBN 0-387-90138-8. - Jech, Thomas (2003),
*Set Theory: The Third Millennium Edition, Revised and Expanded*, Springer Verlag, ISBN 3-540-44085-2 - R. Duncan Luce and Louis Narens (1987). "measurement, theory of,"
*The New Palgrave: A Dictionary of Economics*, v. 3, pp. 428–32. - Luther, Norman Y (1967). "A decomposition of measures".
*Canadian Journal of Mathematics*.**20**: 953–959. doi:10.4153/CJM-1968-092-0. S2CID 124262782. - Mukherjea, A; Pothoven, K (1985).
*Real and Functional Analysis, Part A: Real Analysis*(Second ed.). Plenum Press.- The first edition was published with
*Part B: Functional Analysis*as a single volume: Mukherjea, A; Pothoven, K (1978).*Real and Functional Analysis*(First ed.). Plenum Press. doi:10.1007/978-1-4684-2331-0. ISBN 978-1-4684-2333-4.

- The first edition was published with
- 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. 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) - 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.

In mathematics, specifically in measure theory, a **Borel measure** on a topological space is a measure that is defined on all open sets. Some authors require additional restrictions on the measure, as described below.

In mathematical analysis, a **null set** is a Lebesgue measurable set of real numbers that has **measure zero**. This can be characterized as a set that can be covered by a countable union of intervals of arbitrarily small total length.

In mathematical analysis and in probability theory, a **σ-algebra** on a set *X* is a nonempty collection Σ of subsets of *X* closed under complement, countable unions, and countable intersections. The ordered pair is called a measurable space.

In mathematics, a **complete measure** (or, more precisely, a **complete measure space**) is a measure space in which every subset of every null set is measurable (having measure zero). More formally, a measure space (*X*, Σ, *μ*) is complete if and only if

In mathematics, the ** L^{p} spaces** are function spaces defined using a natural generalization of the

In the mathematical field of real analysis, the **monotone convergence theorem** is any of a number of related theorems proving the convergence of monotonic sequences that are also bounded. Informally, the theorems state that if a sequence is increasing and bounded above by a supremum, then the sequence will converge to the supremum; in the same way, if a sequence is decreasing and is bounded below by an infimum, it will converge to the infimum.

In mathematics, specifically measure theory, the **counting measure** is an intuitive way to put a measure on any set – the "size" of a subset is taken to be the number of elements in the subset if the subset has finitely many elements, and infinity if the subset is infinite.

In mathematics, **Fatou's lemma** establishes an inequality relating the Lebesgue integral of the limit inferior of a sequence of functions to the limit inferior of integrals of these functions. The lemma is named after Pierre Fatou.

In mathematics, the **Radon–Nikodym theorem** is a result in measure theory that expresses the relationship between two measures defined on the same measurable space. A *measure* is a set function that assigns a consistent magnitude to the measurable subsets of a measurable space. Examples of a measure include area and volume, where the subsets are sets of points; or the probability of an event, which is a subset of possible outcomes within a wider probability space.

In mathematics, more precisely in measure theory, an **atom** is a measurable set which has positive measure and contains no set of smaller positive measure. A measure which has no atoms is called **non-atomic** or **atomless**.

In mathematics, the **Bochner integral**, named for Salomon Bochner, extends the definition of Lebesgue integral to functions that take values in a Banach space, as the limit of integrals of simple functions.

In measure theory, **Carathéodory's extension theorem** states that any pre-measure defined on a given ring of subsets *R* of a given set *Ω* can be extended to a measure on the σ-algebra generated by *R*, and this extension is unique if the pre-measure is σ-finite. Consequently, any pre-measure on a ring containing all intervals of real numbers can be extended to the Borel algebra of the set of real numbers. This is an extremely powerful result of measure theory, and leads, for example, to the Lebesgue measure.

In mathematics, a positive (or signed) measure *μ* defined on a *σ*-algebra Σ of subsets of a set *X* is called a finite measure if *μ*(*X*) is a finite real number (rather than ∞), and a set *A* in Σ is of finite measure if *μ*(*A*) < ∞*.* The measure *μ* is called **σ-finite** if *X* is a countable union of measurable sets each with finite measure. A set in a measure space is said to have ** σ-finite measure** if it is a countable union of measurable sets with finite measure. A measure being σ-finite is a weaker condition than being finite, i.e. all finite measures are σ-finite but there are (many) σ-finite measures that are not finite.

**Convergence in measure** is either of two distinct mathematical concepts both of which generalize the concept of convergence in probability.

In mathematics, more precisely in measure theory, a measure on the real line is called a **discrete measure** if it is concentrated on an at most countable set. The support need not be a discrete set. Geometrically, a discrete measure is a collection of point masses.

In mathematics, a **conservative system** is a dynamical system which stands in contrast to a dissipative system. Roughly speaking, such systems have no friction or other mechanism to dissipate the dynamics, and thus, their phase space does not shrink over time. Precisely speaking, they are those dynamical systems that have a null wandering set: under time evolution, no portion of the phase space ever "wanders away", never to be returned to or revisited. Alternately, conservative systems are those to which the Poincaré recurrence theorem applies. An important special case of conservative systems are the measure-preserving dynamical systems.

In probability theory, a **standard probability space**, also called **Lebesgue–Rokhlin probability space** or just **Lebesgue space** is a probability space satisfying certain assumptions introduced by Vladimir Rokhlin in 1940. Informally, it is a probability space consisting of an interval and/or a finite or countable number of atoms.

In measure theory, a branch of mathematics that studies generalized notions of volumes, an **s-finite measure** is a special type of measure. An s-finite measure is more general than a finite measure, but allows one to generalize certain proofs for finite measures.

In mathematics, especially measure theory, a **set function** is a function whose domain is a family of subsets of some given set and that (usually) takes its values in the extended real number line which consists of the real numbers and

In mathematics, **lifting theory** was first introduced by John von Neumann in a pioneering paper from 1931, in which he answered a question raised by Alfréd Haar. The theory was further developed by Dorothy Maharam (1958) and by Alexandra Ionescu Tulcea and Cassius Ionescu Tulcea (1961). Lifting theory was motivated to a large extent by its striking applications. Its development up to 1969 was described in a monograph of the Ionescu Tulceas. Lifting theory continued to develop since then, yielding new results and applications.

- ↑ Fremlin, D. H. (2010),
*Measure Theory*, vol. 2 (Second ed.), p. 221 - 1 2 3 Mukherjea 1985, p. 90.
- ↑ Folland 1999, p. 25.
- ↑ Edgar 1998, Theorem 1.5.2, p. 42.
- ↑ Edgar 1998, Theorem 1.5.3, p. 42.
- 1 2 Nielsen 1997, Exercise 11.30, p. 159.
- ↑ Fremlin 2016, Section 213X, part (c).
- ↑ Royden 2010, Exercise 17.8, p. 342.
- ↑ Hewitt 1965, part (b) of Example 10.4, p. 127.
- ↑ Fremlin 2016, Section 211O, p. 15.
- 1 2 Luther 1967, Theorem 1.
- ↑ Mukherjea 1985, part (b) of Proposition 2.3, p. 90.
- ↑ Fremlin 2016, part (a) of Theorem 243G, p. 159.
- 1 2 Fremlin 2016, Section 243K, p. 162.
- ↑ Fremlin 2016, part (a) of the Theorem in Section 245E, p. 182.
- ↑ Fremlin 2016, Section 245M, p. 188.
- ↑ Berberian 1965, Theorem 39.1, p. 129.
- ↑ Fremlin 2016, part (b) of Theorem 243G, p. 159.
- ↑ Rao, M. M. (2012),
*Random and Vector Measures*, Series on Multivariate Analysis, vol. 9, World Scientific, ISBN 978-981-4350-81-5, MR 2840012 . - ↑ Bhaskara Rao, K. P. S. (1983).
*Theory of charges: a study of finitely additive measures*. M. Bhaskara Rao. London: Academic Press. p. 35. ISBN 0-12-095780-9. OCLC 21196971. - ↑ Folland 1999, p. 27, Exercise 1.15.a.

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