Shift operator

Shift operator

In mathematics, and in particular functional analysis, the shift operators are examples of linear operators, important for their simplicity and natural occurrence. They are used in diverse areas, from Hardy spaces to the theory of abelian varieties.

A typical one-sided shift operator takes an infinite sequence of numbers

(a₁, a₂, ...)

(0, a₁, a₂, ...).

This operation respects typical convergence conditions, such as absolute convergence of the corresponding infinite series; it therefore gives rise to continuous operators on the standard sequence spaces used in functional analysis, usually with norm 1.

Another way to look at it would be in terms of polynomials: the sequences that eventually end in a string

(..., 0, 0, 0, ...)

or, in other words, having only a finite number of non-zero entries, are in a 1-1 correspondence with polynomials in an indeterminate T having a_i as coefficient of Tⁱ. The advantage of this representation is then that the shift operator becomes multiplication by T: this reveals quickly several aspects of its structure. Spaces of polynomials carry numerous topological structures; shift operators can be constructed by extension on corresponding complete spaces.

The bilateral shift operators are the related operators in which the sequences are bi-infinite (functions on the integers, rather than just the natural numbers). One can say that the analogue in this case of the polynomial representation is that by Laurent polynomials. The theory of analytic functions is related to that of polynomials, by allowing infinite power series; on the other hand meromorphic functions have Laurent series that terminate in the direction of negative exponents. In the same way, the one-sided and bilateral shifts have rather different properties.

Action on Hilbert spaces

The unilateral and bilateral shifts have a natural action on Hilbert spaces, giving bounded operators S\ and T on the l^p sequence spaces and respectively. The unilateral shift S is a proper isometry with range equal to all vectors which vanish in the first coordinate. The bilateral shift U, on the other hand, is a unitary operator. The operator S is a compression of U, 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.