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Dirac delta measure : ウィキペディア英語版
Dirac measure

In mathematics, a Dirac measure assigns a size to a set based solely on whether it contains a fixed point ''x'' or not. It is one way of formalizing the idea of the Dirac delta function, an important tool in physics and engineering.
==Definition==
A Dirac measure is a measure ''δ''''x'' on a set ''X'' (with any ''σ''-algebra of subsets of ''X'') defined for a given ''x'' ∈ ''X'' and any (measurable) set ''A'' ⊆ ''X'' by
:\delta_ (A) = 1_A(x)= \begin 0, & x \not \in A; \\ 1, & x \in A. \end
where 1_A is the indicator function of A.
The Dirac measure is a probability measure, and in terms of probability it represents the almost sure outcome ''x'' in the sample space ''X''. We can also say that the measure is a single atom at ''x''; however, treating the Dirac measure as an atomic measure is not correct when we consider the sequential definition of Dirac delta, as the limit of a delta sequence. The Dirac measures are the extreme points of the convex set of probability measures on ''X''.
The name is a back-formation from the Dirac delta function, considered as a Schwartz distribution, for example on the real line; measures can be taken to be a special kind of distribution. The identity
:\int_ f(y) \, \mathrm \delta_ (y) = f(x),
which, in the form
:\int_ f(y) \delta_ (y) \, \mathrm y = f(x),
is often taken to be part of the definition of the "delta function", holds as a theorem of Lebesgue integration.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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