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{{Otheruses4|shift operators in mathematics|operators in computer programming languages|Bitwise operation#Bit shifts}}
In [[mathematics]], and in particular [[functional analysis]], the '''shift operator''' or '''translation operator''' is an operator that takes a function {{math|''f''(''x'')}}
to its '''translation''' {{math|''f''(''x''+''a'')}}.<ref>{{MathWorld|id=ShiftOperator|title=Shift Operator}}</ref> In [[time series analysis]], the shift operator is called the '''[[lag operator]]'''.


Shift operators are examples of [[linear operator]]s, important for their simplicity and natural occurrence. The shift operator action on functions of a real variable plays an important role in [[harmonic analysis]], for example, it appears in the definitions of [[almost periodic function#Uniform or Bohr or Bochner almost periodic functions|almost periodic functions]], [[positive definite function]]s, and [[convolution]].<ref name=mar>{{cite book|mr=2182783|last=Marchenko|first=V. A.|author-link=Vladimir Marchenko|chapter=The generalized shift, transformation operators, and inverse problems|title=Mathematical events of the twentieth century|pages=145&ndash;162|publisher=Springer|location=Berlin|year=2006|doi=10.1007/3-540-29462-7_8}}</ref> Shifts of sequences (functions of an integer variable) appear in diverse areas such as [[Hardy space]]s, the theory of [[abelian variety|abelian varieties]], and the theory of [[symbolic dynamics]], for which the [[baker's map]] is an explicit representation.


==Definition==
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===Functions of a real variable===
 
The shift operator {{math|''T''<sup>''t''</sup>}} ({{math|''t''&nbsp;&isin;&nbsp;'''R'''}}) takes a function {{math|''f''}} on '''R''' to its translation {{math|''f''<sub>''t''</sub>}},  
:<math> f_t(x) = f(x+t)~.</math>
 
A practical representation of the linear operator {{math|''T''<sup>''t''</sup>}} in terms of the plain derivative {{math|<sup>''d''</sup>&frasl;<sub>''dx''</sub>}} was introduced by [[Lagrange]],
:<math>T^t= e^{t \frac{d}{dx}}~, </math>
which may be interpreted operationally through its formal Taylor expansion in ''t''; and whose action on the monomial ''x''<sup>n</sup> is evident by the [[binomial theorem]],  
and thus on all series in ''x''.<ref>Jordan, Charles, (1939/1965). "Calculus of Finite Differences", Chelsea Publishing.</ref>
 
===Sequences===
 
The '''left shift''' operator acts on one-sided [[infinite sequence]] of numbers by
 
:<math> S^*: (a_1, a_2, a_3, \ldots) \mapsto (a_2, a_3, a_4, \ldots)</math>
 
and on two-sided infinite sequences by
 
:<math> T: (a_k)_{k=-\infty}^\infty \mapsto (a_{k+1})_{k=-\infty}^\infty.</math>
 
The '''right shift''' operator acts on one-sided [[infinite sequence]] of numbers by
 
:<math> S: (a_1, a_2, a_3, \ldots) \mapsto (0, a_1, a_2, \ldots)</math>
 
and on two-sided infinite sequences by
 
:<math> T^{-1}:(a_k)_{k=-\infty}^\infty \mapsto (a_{k-1})_{k=-\infty}^\infty.</math>
 
===Abelian groups===
 
In general, if {{math|''f''}} is a function on an [[Abelian group]] {{math|''G''}}, and {{math|''g''}} is an element of {{math|''G''}}, the shift operator {{math|''T''<sup>''g''</sup>}} maps {{math|''f''}} to
 
:<math> f_g(h) = f(g+h).</math><ref>{{eom|id=S/s084900|last=Millionshchikov|first=V.M.}}</ref>
 
==Properties of the shift operator==
 
The shift operator acting on real- or complex-valued functions or sequences is a linear operator which preserves most of the standard [[norm (mathematics)|norms]] which appear in functional analysis. Therefore it is usually a [[continuous  operator]] with norm one.
 
===Action on Hilbert spaces===
 
The shift operator acting on two-sided sequences is a [[unitary operator]] on  {{math|''l''<sub>2</sub>('''Z''')}}. The shift operator acting on functions of a real variable is a unitary operator on {{math|''L''<sub>2</sub>('''R''')}}.
 
In both cases, the (left) shift operator satisfies the following commutation relation with the Fourier transform:
 
:<math> \mathcal{F} T^t = M^t \mathcal{F}, </math>
 
where {{math|''M''<sup>''t''</sup>}} is the [[multiplication operator]] by {{math|exp(i ''t''  ''x'')}}. Therefore the spectrum of {{math|''T''<sup>''t''</sup>}} is the unit circle.
 
The one-sided shift {{math|''S''}} acting on {{math|''l''<sub>2</sub>('''N''')}} is a proper [[isometry]] with [[range (mathematics)|range]] equal to all [[Vector (geometric)|vectors]] which vanish in the first [[coordinate]]. The operator ''S'' is a [[compression (functional analysis)|compression]] of ''T<sup>&minus;1</sup>'', in the sense that
 
:<math>T^{-1}y=Sx \text{ for each } x \in \ell^2(\mathbb{N}),\,</math>
 
where {{math|''y''}} is the vector in {{math|''l''<sub>2</sub>('''Z''')}} with {{math|''y''<sub>''i''</sub>}}&nbsp;=&nbsp;{{math|''x''<sub>''i''</sub>}} for {{math|''i''&nbsp;&ge;&nbsp;0}} and {{math|''y''<sub>''i''</sub>}}&nbsp;=&nbsp;{{math|0}} for {{math|''i''&nbsp;<&nbsp;0}}. This observation is at the heart of the construction of many [[unitary dilation]]s of isometries.
 
The spectrum of ''S'' is the unit disk. The shift ''S'' is one example of a [[Fredholm operator]]; it has Fredholm index&nbsp;&minus;1.
 
==Generalisation==
 
[[Jean Delsarte]] introduced the notion of '''generalised shift operator''' (also called '''generalised displacement operator'''); it was further developed by [[Boris Levitan]].<ref name = mar/><ref>{{SpringerEOM|id=g/g043800|first=B.M.|last=Levitan|author-link=Boris Levitan|first2=G.L.|last2=Litvinov|title=Generalized displacement operators}}</ref><ref>{{SpringerEOM|id=A/a011970|first=E.A.|last= Bredikhina|title=Almost-periodic function}}</ref>
 
A family of operators {{math|{''L''<sup>''x''</sup>}<sub>''x''&nbsp;&isin;&nbsp;''X''</sub>}} acting on a space {{math|''&Phi;''}} of functions from a set {{math|''X''}} to {{math|'''C'''}} is called a family of generalised shift operators if the following properties hold:
# Associativity: let {{math|(''R''<sup>''y''</sup>''f'')(''x'')}}&nbsp;=&nbsp;{{math|(''L''<sup>''x''</sup>''f'')(''y'')}}. Then {{math|''L''<sup>''x''</sup>''R''<sup>''y''</sup>}}&nbsp;=&nbsp;{{math|''R''<sup>''y''</sup>''L''<sup>''x''</sup>}}.
# There exists {{math|''e''&nbsp;&isin;&nbsp;''X''}} such that {{math|''L''<sup>''e''</sup>}} is the identity operator.
In this case, the set {{math|'''X'''}} is called a [[hypergroup]].
 
==See also==
*[[Arithmetic shift]]
*[[Logical shift]]
*[[Finite_difference#Calculus_of_finite_differences|Finite difference]]
 
==Notes==
{{Reflist}}
 
==Bibliography==
* Jonathan R. Partington, ''Linear Operators and Linear Systems, An Analytical Approach to Control Theory'', (2004) London Mathematical Society Student Texts '''60''', Cambridge University Press.
* Marvin Rosenblum and James Rovnyak, ''Hardy Classes and Operator Theory'', (1985) Oxford University Press.
 
{{DEFAULTSORT:Shift Operator}}
[[Category:Unitary operators]]
[[Category:Isometric operators]]

Revision as of 02:36, 28 February 2014


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