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In [[mathematics]], particularly [[linear algebra]], an '''orthonormal basis''' for an [[inner product space]] ''V'' with finite [[dimension (linear algebra)|dimension]] is a [[Basis (linear algebra)|basis]] for ''V'' whose vectors are [[orthonormal]].<ref>{{cite book | last=Lay | first=David C. | title=Linear Algebra and Its Applications | publisher=[[Addison–Wesley]] | year=2006 | edition = 3rd | isbn=0-321-28713-4}}</ref><ref>{{cite book | last=Strang | first=Gilbert | authorlink=Gilbert Strang | title=Linear Algebra and Its Applications | publisher=[[Brooks Cole]] | year=2006 | edition = 4th | isbn=0-03-010567-6}}</ref><ref>{{cite book | last = Axler | first = Sheldon | title = Linear Algebra Done Right | publisher = [[Springer Science+Business Media|Springer]] | year = 2002 | edition = 2nd | isbn = 0-387-98258-2}}</ref>  For example, the [[standard basis]] for an [[Euclidean space]] '''R'''<sup>''n''</sup> is an orthonormal basis, where the relevant inner product is the [[dot product]] of vectors.  The [[Image (mathematics)|image]] of the standard basis under a [[rotation (mathematics)|rotation]] or [[reflection (mathematics)|reflection]] (or any [[orthogonal transformation]]) is also orthonormal, and every orthonormal basis for '''R'''<sup>''n''</sup> arises in this fashion.
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For a general inner product space ''V'', an orthonormal basis can be used to define normalized [[orthogonal coordinates]] on ''V''.  Under these coordinates, the inner product becomes dot product of vectors. Thus the presence of an orthonormal basis reduces the study of a [[Dimension (vector space)|finite-dimensional]] inner product space to the study of '''R'''<sup>''n''</sup> under dot product.  Every finite-dimensional inner product space has an orthonormal basis, which may be obtained from an arbitrary basis using the [[Gram–Schmidt process]].
 
In [[functional analysis]], the concept of an orthonormal basis can be generalized to arbitrary (infinite-dimensional) inner product spaces (or [[pre-Hilbert space]]s).<ref>{{cite book | last=Rudin | first=Walter | authorlink=Walter Rudin | title=Real & Complex Analysis | publisher=[[McGraw-Hill]] | year=1987 | isbn=0-07-054234-1}}</ref> Given a pre-Hilbert space ''H'', an orthonormal basis for ''H'' is an orthonormal set of vectors with the property that every vector in ''H'' can be written as an [[infinite linear combination]] of the vectors in the basis.  In this case, the orthonormal basis is sometimes called a '''Hilbert basis''' for ''H''.  Note that an orthonormal basis in this sense is not generally a [[Hamel basis]], since infinite linear combinations are required.  Specifically, the [[linear span]] of the basis must be [[Dense set|dense]] in ''H'', but it may not be the entire space.
 
==Examples==
* The set of vectors {''e''<sub>1</sub>&nbsp;=&nbsp;(1,&nbsp;0,&nbsp;0), ''e''<sub>2</sub>&nbsp;=&nbsp;(0,&nbsp;1,&nbsp;0), ''e''<sub>3</sub>&nbsp;=&nbsp;(0,&nbsp;0,&nbsp;1)} (the standard basis) forms an orthonormal basis of '''R'''<sup>3</sup>.
::'''Proof:''' A straightforward computation shows that the inner products of these vectors equals zero, &lt;''e''<sub>1</sub>, ''e''<sub>2</sub>&gt; = &lt;''e''<sub>1</sub>, ''e''<sub>3</sub>&gt; = &lt;''e''<sub>2</sub>, ''e''<sub>3</sub>&gt; = 0 and that each of their magnitudes equals one, ||''e''<sub>1</sub>|| = ||''e''<sub>2</sub>|| = ||''e''<sub>3</sub>|| = 1. This means {''e''<sub>1</sub>, ''e''<sub>2</sub>, ''e''<sub>3</sub>} is an orthonormal set. All vectors (''x'',&nbsp;''y'',&nbsp;''z'') in '''R'''<sup>3</sup> can be expressed as a sum of the basis vectors scaled
:::<math> (x,y,z) = xe_1 + ye_2 + ze_3, \, </math>
::so {''e''<sub>1</sub>,''e''<sub>2</sub>,''e''<sub>3</sub>} spans '''R'''<sup>3</sup> and hence must be a basis. It may also be shown that the standard basis rotated about an axis through the origin or reflected in a plane through the origin forms an orthonormal basis of '''R'''<sup>3</sup>.
* The set {''f''<sub>''n''</sub> : ''n'' ∈ '''Z'''} with ''f''<sub>''n''</sub>(''x'') = [[exponential function|exp]](2π''inx'') forms an orthonormal basis of the space of functions with finite Lebesgue integrals, L<sup>2</sup>([0,1]), with respect to the [[2 norm]]. This is fundamental to the study of [[Fourier series]].
* The set {''e''<sub>''b''</sub> : ''b'' ∈ ''B''} with ''e''<sub>''b''</sub>(''c'')&nbsp;=&nbsp;1 if ''b''&nbsp;=&nbsp;''c'' and 0 otherwise forms an orthonormal basis of ''ℓ''<sup>&nbsp;2</sup>(''B'').
* Eigenfunctions of a [[Sturm–Liouville eigenproblem]].
* An [[orthogonal matrix]] is a matrix whose column vectors form an orthonormal set.
 
==Basic formula==
If ''B'' is an orthogonal basis of ''H'', then every element ''x'' of ''H'' may be written as
 
:<math>x=\sum_{b\in B}{\langle x,b\rangle\over\lVert b\rVert^2} b.</math>
 
When ''B'' is orthonormal, we have instead
 
:<math>x=\sum_{b\in B}\langle x,b\rangle b</math>
 
and the [[norm (mathematics)|norm]] of ''x'' can be given by
 
:<math>\|x\|^2=\sum_{b\in B}|\langle x,b\rangle |^2.</math>
 
Even if ''B'' is [[Uncountable set|uncountable]], only countably many terms in this sum will be non-zero, and the expression is therefore well-defined. This sum is also called the ''Fourier expansion'' of ''x'', and the formula is usually known as [[Parseval's identity]]. See also [[Generalized Fourier series]].
 
If ''B'' is an orthonormal basis of ''H'', then ''H'' is ''isomorphic'' to ''ℓ''<sup>&nbsp;2</sup>(''B'') in the following sense: there exists a [[bijective]] [[linear operator|linear]] map {{nowrap|Φ : ''H'' → ''ℓ''<sup> 2</sup>(''B'')}} such that
 
:<math>\langle\Phi(x),\Phi(y)\rangle=\langle x,y\rangle</math>
 
for all ''x'' and ''y'' in ''H''.
 
==Incomplete orthogonal sets==
Given a Hilbert space ''H'' and a set ''S'' of mutually orthogonal vectors in ''H'', we can take the smallest closed linear subspace ''V'' of ''H'' containing ''S''. Then ''S'' will be an orthogonal basis of ''V''; which may of course be smaller than ''H'' itself, being an ''incomplete'' orthogonal set, or be ''H'', when it is a ''complete'' orthogonal set.
 
==Existence==
Using [[Zorns lemma|Zorn's lemma]] and the [[Gram–Schmidt process]] (or more simply well-ordering and transfinite recursion), one can show that ''every'' Hilbert space admits a basis and thus an orthonormal basis; furthermore, any two orthonormal bases of the same space have the same [[cardinal number|cardinality]] (this can be proven in a manner akin to that of the proof of the usual [[dimension theorem for vector spaces]], with separate cases depending on whether  the larger basis candidate is countable or not). A Hilbert space is [[separable metric space|separable]] if and only if it admits a [[countable]] orthonormal basis. (One can prove this last statement without using the axiom of choice).
 
==As a homogeneous space==
{{Main|Stiefel manifold}}
The set of orthonormal bases for a space is a [[principal homogeneous space]] for the [[orthogonal group]] O(''n''), and is called the [[Stiefel manifold]] <math>V_n(\mathbf{R}^n)</math> of orthonormal [[k-frame|''n''-frames]].
 
In other words, the space of orthonormal bases is like the orthogonal group, but without a choice of base point: given an orthogonal space, there is no natural choice of orthonormal basis, but once one is given one, there is a one-to-one correspondence between bases and the orthogonal group.
Concretely, a linear map is determined by where it sends a given basis: just as an invertible map can take any basis to any other basis, an orthogonal map can take any ''orthogonal'' basis to any other ''orthogonal'' basis.
 
The other Stiefel manifolds <math>V_k(\mathbf{R}^n)</math> for <math>k < n</math> of ''incomplete'' orthonormal bases (orthonormal ''k''-frames) are still homogeneous spaces for the orthogonal group, but not ''principal'' homogeneous spaces: any ''k''-frame can be taken to any other ''k''-frame by an orthogonal map, but this map is not uniquely determined.
 
==See also==
*[[Basis (linear algebra)]]
*[[Schauder basis]]
 
==References==
{{reflist}}
 
{{DEFAULTSORT:Orthonormal Basis}}
[[Category:Linear algebra]]
[[Category:Functional analysis]]
[[Category:Fourier analysis]]

Latest revision as of 18:44, 4 September 2014

The initially popular kind are the creams and ointments where we rub a drugs onto the outside of the rectum. It intends to treat your hemorrhoid by soothing the blood vessels. This relaxes the cells so that it no longer continues to bulge. Once the tissues go down, the hemorrhoids may not flare up as much. This really is great for a little temporary relief, yet the hemorrhoid might normally flare up again whenever utilizing this method of primary treatment.

Before you finally find out the greatest how to stop bleeding hemorrhoids, it is actually significant to understand initially the cause of the hemorrhoid. Actually there are many causes of hemorrhoid including irregularity, prolong sitting or standing, pregnancy along with a lot more. The initially thing that you require to do is to cure the cause and for sure getting rid of the hemorrhoid usually follow.

More fiber in a diet is how to get rid of hemorrhoids so which they may remain inactive. Eat a lot of fruits and vegetables, and when necessary take a fiber supplement to make sure you're getting all of the fiber you require. Hemorrhoids thrive off of inactivity, plus various individuals that are bound to chairs or beds suffer from hemorrhoids. If it happens to be possible for we to be less sedentary, then do thus. Getting enough fiber in a diet plus getting standard exercise will greatly minimize the hemorrhoids that are creating we suffer.

If you will ask wellness practitioners they usually recommend surgery inside getting rid of your hemorrhoid. The procedures in operation are fairly simple plus to receive out o the painful condition once you are completed treating it.

Witch Hazel: you are able to use witch hazel straight to the swelling. Just put several witch hazel on some cotton plus apply it directly to the hemorrhoids. This will greatly reduce the swelling of the veins.

One of the points which usually certainly make hemorrhoids worse is should you stress a lot whilst going to the bathroom. It is significant today you are having certain soft stool, if your stool is hard then you'll be straining. The easiest way to make sure it is very soft is to consume foods which are especially significant in fiber.

The main solution we would desire to discover out is if it does function or not and where may i buy venapro. Survey carried out by independent organizations reveal which it works also as the top amidst the other hemorrhoid treatment products. It will reduce plus heal the infected skin using its elements.