The shift operator takes a function on R to its translation , A practical representation of the linear operator in terms of the plain derivative was introduced by Lagrange, which may be interpreted operationally through its formal Taylor expansion in ; and whose action on the monomial is evident by the binomial theorem, and hence on all series in, and so all functions as above. This, then, is a formal encoding of the Taylor expansion. The operator thus provides the prototype for Lie's celebrated advective flow for Abelian groups, where the canonical coordinates are defined, s.t. For example, it easily follows that yields scaling, hence ; likewise, yields yields yields etc. The initial condition of the flow and the group property completely determine the entire Lie flow, providing a solution to the translation functional equation
Sequences
The left shift operator acts on one-sided infinite sequence of numbers by and on two-sided infinite sequences by The right shift operator acts on one-sided infinite sequence of numbers by and on two-sided infinite sequences by The right and left shift operators acting on two-sided infinite sequences are called bilateral shifts.
The shift operator acting on real- or complex-valued functions or sequences is a linear operator which preserves most of the standard norms which appear in functional analysis. Therefore, it is usually a continuous operator with norm one.
The shift operator acting on two-sided sequences is a unitary operator on . The shift operator acting on functions of a real variable is a unitary operator on. In both cases, the shift operator satisfies the following commutation relation with the Fourier transform: where is the multiplication operator by. Therefore, the spectrum of is the unit circle. The one-sided shift acting on is a proper isometry with rangeequal to all vectors which vanish in the first coordinate. The operator S is a compression of T−1, in the sense that where is the vector in with = for and = for. This observation is at the heart of the construction of many unitary dilations of isometries. The spectrum of S is the unit disk. The shift S is one example of a Fredholm operator; it has Fredholm index −1.
Generalisation
introduced the notion of generalised shift operator ; it was further developed by Boris Levitan. A family of operators acting on a space of functions from a set to is called a family of generalised shift operators if the following properties hold: