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Orthogonal basis

From Wikipedia, the free encyclopedia
Basis consisting of mutually orthogonal vectors

Inmathematics, particularlylinear algebra, anorthogonal basis for aninner product spaceV{\displaystyle V} is abasis forV{\displaystyle V} whose vectors are mutuallyorthogonal. If the vectors of an orthogonal basis arenormalized, the resulting basis is anorthonormal basis.

As coordinates

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Any orthogonal basis can be used to define a system oforthogonal coordinatesV.{\displaystyle V.} Orthogonal (not necessarily orthonormal) bases are important due to their appearance fromcurvilinear orthogonal coordinates inEuclidean spaces, as well as inRiemannian andpseudo-Riemannian manifolds.

In functional analysis

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Infunctional analysis, an orthogonal basis is any basis obtained from an orthonormal basis (or Hilbert basis) using multiplication by nonzeroscalars.

Extensions

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Symmetric bilinear form

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The concept of an orthogonal basis is applicable to avector spaceV{\displaystyle V} (over anyfield) equipped with asymmetric bilinear form,{\displaystyle \langle \cdot ,\cdot \rangle }, whereorthogonality of two vectorsv{\displaystyle v} andw{\displaystyle w} meansv,w=0{\displaystyle \langle v,w\rangle =0}. For an orthogonal basis{ek}{\displaystyle \left\{e_{k}\right\}}:ej,ek={q(ek)j=k0jk,{\displaystyle \langle e_{j},e_{k}\rangle ={\begin{cases}q(e_{k})&j=k\\0&j\neq k,\end{cases}}}whereq{\displaystyle q} is aquadratic form associated with,:{\displaystyle \langle \cdot ,\cdot \rangle :}q(v)=v,v{\displaystyle q(v)=\langle v,v\rangle } (in an inner product space,q(v)=v2{\displaystyle q(v)=\Vert v\Vert ^{2}}).

Hence for an orthogonal basis{ek}{\displaystyle \left\{e_{k}\right\}},v,w=kq(ek)vkwk,{\displaystyle \langle v,w\rangle =\sum _{k}q(e_{k})v_{k}w_{k},}wherevk{\displaystyle v_{k}} andwk{\displaystyle w_{k}} are components ofv{\displaystyle v} andw{\displaystyle w} in the basis.

Quadratic form

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The concept of orthogonality may be extended to a vector space over any field of characteristic not 2 equipped with a quadratic formq(v){\displaystyle q(v)}. Starting from the observation that, when the characteristic of the underlying field is not 2, the associated symmetric bilinear formv,w=12(q(v+w)q(v)q(w)){\displaystyle \langle v,w\triangle ={\tfrac {1}{2}}(q(v+w)-q(v)-q(w))} allows vectorsv{\displaystyle v} andw{\displaystyle w} to be defined as being orthogonal with respect toq{\displaystyle q} whenq(v+w)q(v)q(w)=0{\displaystyle q(v+w)-q(v)-q(w)=0}.

See also

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References

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External links

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