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{{Hatnote|For unitarity in physics, see [[Unitarity (physics)]].}}


In [[functional analysis]], a branch of [[mathematics]], a '''unitary operator''' (not to be confused with a unity operator) is a [[bounded linear operator]] ''U'' : ''H'' → ''H'' on a [[Hilbert space]] ''H'' satisfying


:<math>U^*U=UU^*=I \!</math>
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where ''U''<sup></sup> is the [[Hermitian adjoint|adjoint]] of ''U'', and ''I''&nbsp;:&nbsp;''H''&nbsp;→&nbsp;''H'' is the [[identity (mathematics)|identity]] operator. This property is equivalent to the following:
 
#''U'' preserves the [[inner product]] 〈&nbsp; , &nbsp;〉 of the Hilbert space, i.e., for all [[vector space|vector]]s ''x'' and ''y'' in the Hilbert space, <math>\langle Ux, Uy \rangle = \langle x, y \rangle</math>, and
#''U'' is [[surjective function|surjective]].  
 
It is also equivalent to the seemingly weaker condition:
 
#''U'' preserves the [[inner product]], and
#the range of ''U'' is [[dense set|dense]].
 
To see this, notice that ''U'' preserves the inner product implies ''U'' is an [[isometry]] (thus, a [[bounded linear operator]]). The fact that ''U'' has dense range ensures it has a bounded inverse ''U''<sup>&minus;1</sup>. It is clear that ''U''<sup>&minus;1</sup> = ''U''<sup>∗</sup>. 
 
Thus, unitary operators are just [[automorphism]]s of [[Hilbert space]]s, i.e., they preserve the structure (in this case, the linear space structure, the inner product, and hence the [[topology]]) of the space on which they act. The [[group (mathematics)|group]] of all unitary operators from a given Hilbert space ''H'' to itself is sometimes referred to as the '''Hilbert group''' of ''H'', denoted Hilb(''H'').
 
The weaker condition ''U''<sup></sup>''U''&nbsp;=&nbsp;''I'' defines an ''isometry''. Another condition, ''U'' ''U''<sup></sup>&nbsp;=&nbsp;''I'', defines a ''coisometry''.<ref>{{harv|Halmos|1982|loc=Sect. 127, page 69}}</ref>
 
A '''unitary element''' is a generalization of a unitary operator. In a [[unital algebra|unital]] [[*-algebra]], an element ''U'' of the algebra is called a unitary element if  
:<math>U^*U=UU^*=I</math>
where ''I'' is the identity element.<ref>
{{cite book | last = Doran | first = Robert S. |coauthors = Victor A. Belfi | title = Characterizations of C*-Algebras: The Gelfand-Naimark Theorems | publisher = Marcel Dekker | location = New York | year = 1986 | isbn = 0-8247-7569-4 }}
</ref>{{Rp|55}}
 
==Examples==
 
* The [[identity function]] is trivially a unitary operator.
 
* Rotations in '''R'''<sup>''2''</sup> are the simplest nontrivial example of unitary operators. Rotations do not change the length of a vector or the angle between 2 vectors. This example can be expanded to '''R'''<sup>''3''</sup>.
 
* On the [[vector space]] '''C''' of [[complex number]]s, multiplication by a number of [[absolute value]] 1, that is, a number of the form ''e''<sup>''i θ''</sup> for ''θ'' ∈ '''R''', is a unitary operator.  ''θ'' is referred to as a phase, and this multiplication is referred to as multiplication by a phase.  Notice that the value of ''θ'' modulo 2''π'' does not affect the result of the multiplication, and so the independent unitary operators on '''C''' are parametrized by a circle. The corresponding group, which, as a set, is the circle, is called U(1).
 
* More generally, [[unitary matrix|unitary matrices]] are precisely the unitary operators on finite-dimensional [[Hilbert space]]s, so the notion of a unitary operator is a generalization of the notion of a unitary matrix.  [[Orthogonal matrix|Orthogonal matrices]] are the special case of unitary matrices in which all entries are real. They are the unitary operators on '''R'''<sup>''n''</sup>.
 
* The [[bilateral shift]] on the [[Lp space|sequence space]] <math>\ell^2</math> indexed by the [[integer]]s is unitary. In general, any operator in a Hilbert space which acts by shuffling around an [[orthonormal basis]] is unitary. In the finite dimensional case, such operators are the [[permutation matrix|permutation matrices]]. The [[unilateral shift]] is an isometry; its conjugate is a coisometry.
 
* The [[Fourier operator]] is a unitary operator, i.e. the operator which performs the [[Fourier transform]] (with proper normalization). This follows from [[Parseval's theorem]].
 
* Unitary operators are used in [[unitary representation]]s.
 
==Linearity==
 
The linearity requirement in the definition of a unitary operator can be dropped without changing the meaning because it can be derived from linearity and positive-definiteness of the [[scalar product]]:
:<math> \langle \lambda\cdot Ux-U(\lambda\cdot x), \lambda\cdot Ux-U(\lambda\cdot x) \rangle </math>
:<math>  = \| \lambda \cdot Ux \|^2 + \| U(\lambda \cdot x) \|^2 - \langle U(\lambda\cdot x), \lambda\cdot Ux \rangle - \langle \lambda\cdot Ux, U(\lambda\cdot x) \rangle </math>
:<math> = |\lambda|^2 \cdot \| Ux \|^2 + \| U(\lambda \cdot x) \|^2 - \overline{\lambda}\cdot \langle U(\lambda\cdot x), Ux \rangle - \lambda\cdot \langle Ux, U(\lambda\cdot x) \rangle </math>
:<math> = |\lambda|^2 \cdot \| x \|^2 + \| \lambda \cdot x \|^2 - \overline{\lambda}\cdot \langle \lambda\cdot x, x \rangle - \lambda\cdot \langle x, \lambda\cdot x \rangle </math>
:<math> = 0</math>
:Analogously you obtain <math>\langle U(x+y)-(Ux+Uy), U(x+y)-(Ux+Uy) \rangle = 0 </math>.
 
==Properties==
 
* The [[spectrum (functional analysis)|spectrum]] of a unitary operator ''U'' lies on the unit circle. That is, for any complex number λ in the spectrum, one has |λ|=1. This can be seen as a consequence of the [[spectral theorem]] for [[normal operator]]s. By the theorem, ''U'' is unitarily equivalent to multiplication by a Borel-measurable ''f'' on ''L''²(''μ''), for some finite measure space (''X'', ''μ''). Now ''U U*'' = ''I'' implies |''f''(''x'')|² = 1 ''μ''-a.e. This shows that the essential range of ''f'', therefore the spectrum of ''U'', lies on the unit circle.
 
==See also==
*[[Unitary matrix]]
*[[Unitary transformation]]
*[[Antiunitary]]
 
==Footnotes==
{{Reflist}}
 
==References==
 
* {{cite book
| authorlink=Serge Lang
|      last = Lang
|    first = Serge
|    title = Differential manifolds
| publisher = Addison-Wesley Publishing Co., Inc.  
|  location = Reading, Mass.&ndash;London&ndash;Don Mills, Ont.  
|      year = 1972
}}
* {{cite book
| authorlink=Paul Halmos
| last = Halmos
| first = Paul
| title = A Hilbert space problem book
| publisher = Springer
| year = 1982
}}
 
{{Functional Analysis}}
 
[[Category:Operator theory]]
[[Category:Unitary operators]]
 
[[de:Unitäre Abbildung]]

Latest revision as of 05:47, 17 November 2014




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The following are important points which have learned from multiple startup operations that utilize offshore IT resources. Follow these tips for success discover ways to dramatically chances for success.

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