Almost Nowhere

In measure theory (a branch of mathematical analysis), a property holds almost everywhere if, in a technical sense, the set for which the property holds takes up nearly all possibilities. The notion of "almost everywhere" is a companion notion to the concept of measure zero, and is analogous to the notion of ''almost surely'' in probability theory.

More specifically, a property holds almost everywhere if it holds for all elements in a set except a subset of measure zero, or equivalently, if the set of elements for which the property holds is conull. In cases where the measure is not complete, it is sufficient that the set be contained within a set of measure zero. When discussing sets of real numbers, the Lebesgue measure is usually assumed unless otherwise stated.

The term ''almost everywhere'' is abbreviated ''a.e.''; in older literature ''p.p.'' is used, to stand for the equivalent French language phrase ''presque partout''.

A set with full measure is one whose complement is of measure zero. In probability theory, the terms ''almost surely'', ''almost certain'' and ''almost always'' refer to events with probability 1 not necessarily including all of the outcomes. These are exactly the sets of full measure in a probability space.

Occasionally, instead of saying that a property holds almost everywhere, it is said that the property holds for almost all elements (though the term almost all can also have other meanings).

Definition

If $(X,\Sigma,\mu)$ is a measure space, a property $P$ is said to hold almost everywhere in $X$ if there exists a measurable set $N \in \Sigma$ with $\mu(N) = 0$, and all $x\in X\setminus N$ have the property $P$.
Another common way of expressing the same thing is to say that "almost every point satisfies $P\,$", or that "for almost every $x$, $P(x)$ holds".

It is ''not'' required that the set $\$ has measure zero; it may not be measurable.
By the above definition, it is sufficient that $\$ be contained in some set $N$ that is measurable and has measure zero.
However, this technicality vanishes when considering a complete measure space: if $X$ is complete then $N$ exists with measure zero if and only if $\$ is measurable with measure zero.

Properties

* If property $P$ holds almost everywhere and implies property ''$Q$'', then property ''$Q$'' holds almost everywhere. This follows from the monotonicity of measures.
* If $(P_n)$ is a finite or a countable sequence of properties, each of which holds almost everywhere, then their conjunction $\forall n P_n$ holds almost everywhere. This follows from the countable sub-additivity of measures.
* By contrast, if $(P_x)_$ is an uncountable family of properties, each of which holds almost everywhere, then their conjunction $\forall x P_x$ does not necessarily hold almost everywhere. For example, if $\mu$ is Lebesgue measure on $X = \mathbf R$ and $P_x$ is the property of not being equal to $x$ (i.e. $P_x(y)$ is true if and only if $y \neq x$), then each $P_x$ holds almost everywhere, but the conjunction $\forall x P_x$ does not hold anywhere.

As a consequence of the first two properties, it is often possible to reason about "almost every point" of a measure space as though it were an ordinary point rather than an abstraction. This is often done implicitly in informal mathematical arguments. However, one must be careful with this mode of reasoning because of the third bullet above: universal quantification over uncountable families of statements is valid for ordinary points but not for "almost every point".

Examples

* If ''f'' : R → R is a Lebesgue integrable function and $f(x) \ge 0$ almost everywhere, then $\int_a^b f(x) \, dx \geq 0$ for all real numbers $a < b$ with equality if and only if $f(x) = 0$ almost everywhere.
* If ''f'' : 'a'', ''b''→ R is a monotonic function, then ''f'' is differentiable almost everywhere.
* If ''f'' : R → R is Lebesgue measurable and $\int_a^b , f(x), \, dx < \infty$ for all real numbers $a < b$, then there exists a set ''E'' (depending on ''f'') such that, if ''x'' is in ''E'', the Lebesgue mean $\frac \int_^ f(t)\,dt$ converges to as $\epsilon$ decreases to zero. The set ''E'' is called the Lebesgue set of ''f''. Its complement can be proved to have measure zero. In other words, the Lebesgue mean of ''f'' converges to ''f'' almost everywhere.
* A bounded function is Riemann integrable if and only if it is continuous almost everywhere.
* As a curiosity, the decimal expansion of almost every real number in the interval , 1contains the complete text of Shakespeare's plays, encoded in ASCII; similarly for every other finite digit sequence, see Normal number.

Definition using ultrafilters

Outside of the context of real analysis, the notion of a property true almost everywhere is sometimes defined in terms of an ultrafilter. An ultrafilter on a set ''X'' is a maximal collection ''F'' of subsets of ''X'' such that:
# If ''U'' ∈ ''F'' and ''U'' ⊆ ''V'' then ''V'' ∈ ''F''
# The intersection of any two sets in ''F'' is in ''F''
# The empty set is not in ''F''
A property ''P'' of points in ''X'' holds almost everywhere, relative to an ultrafilter ''F'', if the set of points for which ''P'' holds is in ''F''.

For example, one construction of the hyperreal number system defines a hyperreal number as an equivalence class of sequences that are equal almost everywhere as defined by an ultrafilter.

The definition of ''almost everywhere'' in terms of ultrafilters is closely related to the definition in terms of measures, because each ultrafilter defines a finitely-additive measure taking only the values 0 and 1, where a set has measure 1 if and only if it is included in the ultrafilter.

See also

* Dirichlet's function, a function that is equal to 0 almost everywhere.

References

Bibliography

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{{Lp spaces

Mathematical terminology
Measure theory

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