<?xml version="1.0" encoding="UTF-8"?>

<record version="16" id="5346">
 <title>orthonormal basis</title>
 <name>OrthonormalBasis</name>
 <created>2003-10-15 01:32:21</created>
 <modified>2008-03-21 14:09:02</modified>
 <type>Definition</type>
 <creator id="2760" name="yark"/>
 <author id="2760" name="yark"/>
 <author id="3284" name="apmxi"/>
 <author id="932" name="say_10"/>
 <author id="3" name="drini"/>
 <classification>
	<category scheme="msc" code="46C05"/>
 </classification>
 <defines>
	<concept>dimension of a Hilbert space</concept>
	<concept>dimension</concept>
 </defines>
 <synonyms>
	<synonym concept="orthonormal basis" alias="Hilbert basis"/>
 </synonyms>
 <related>
	<object name="RieszSequence"/>
	<object name="Orthonormal"/>
	<object name="ClassificationOfHilbertSpaces"/>
 </related>
 <preamble>\def\ip#1{{\langle #1\rangle}}
</preamble>
 <content>\PMlinkescapeword{even}
\PMlinkescapeword{finite}
\PMlinkescapeword{terms}
\PMlinkescapeword{properties}

\section*{Definition}

An \emph{orthonormal basis} (or \emph{Hilbert basis})
of an inner product space $V$
is a subset $B$ of $V$ satisfying the following two properties:
\begin{itemize}
\item $B$ is an orthonormal set.
\item The linear span of $B$ is dense in $V$.
\end{itemize}

The first condition means that all elements of $B$ have norm $1$
and every element of $B$ is \PMlinkname{orthogonal}{OrthogonalVectors} to every other element of $B$.
The second condition says that every element of $V$ can be approximated arbitrarily closely by (finite) linear combinations of elements of $B$.

\section*{Orthonormal bases of Hilbert spaces}

Every Hilbert space has an orthonormal basis.
The cardinality of this orthonormal basis
is called the \emph{dimension} of the Hilbert space.
(This is well-defined,
as the cardinality does not depend on the choice of orthonormal basis.
This dimension is not in general the same as
\PMlinkname{the usual concept of dimension for vector spaces}{Dimension2}.)

If $B$ is an orthonormal basis of a Hilbert space $H$,
then for every $x\in H$ we have
\[
  x=\sum_{b\in B}\ip{x,b}b.
\]
Thus $x$ is expressed as a (possibly infinite)
``linear combination'' of elements of $B$.
The expression is well-defined,
because only countably many of the terms $\ip{x,b}b$ are non-zero
(even if $B$ itself is uncountable),
and if there are infinitely many non-zero terms
the series is unconditionally convergent.
For any $x,y\in H$ we also have
\[
  \ip{x,y}=\sum_{b\in B}\ip{x,b}\ip{b,y}.
\]
</content>
</record>
