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Stationary Process Invertibility and the Unilateral Shift Operator

Anand Ganesh, Babhrubahan Bose, Anand Rajagopalan

Abstract

The bilateral shift operator $B$ has been the mainstay of stationary process modeling whereas we argue that the unilateral shift operator $T$ may be better suited to analyze invertibility. While doing so, we partially unify the notion of stationary process invertibility (associated with a sufficent but not necessary $\ell^1$ condition) with the algebraic invertibility of the transfer function $f(T)$. We establish a rigorous operator theoretic foundation for these arguments proving that for $f \in \mathbb{W}_+$, the Wiener algebra, $f(T)$ is well defined, that $\| f(T) \| = \| f \|_{\infty}$ and that $f(T) = T_f$, the Toeplitz operator.

Stationary Process Invertibility and the Unilateral Shift Operator

Abstract

The bilateral shift operator has been the mainstay of stationary process modeling whereas we argue that the unilateral shift operator may be better suited to analyze invertibility. While doing so, we partially unify the notion of stationary process invertibility (associated with a sufficent but not necessary condition) with the algebraic invertibility of the transfer function . We establish a rigorous operator theoretic foundation for these arguments proving that for , the Wiener algebra, is well defined, that and that , the Toeplitz operator.

Paper Structure

This paper contains 5 sections, 6 theorems, 16 equations.

Key Result

Theorem 1

Wold DecompositionHamilton1994: Any zero-mean covariance-stationary process $X_t$ can be represented in the form $\blacktriangleleft$$\blacktriangleleft$

Theorems & Definitions (13)

  • Definition 1: Unilateral and Bilateral Shift Operators
  • Definition 2: Wiener Algebra
  • Definition 3: Stationary Process
  • Theorem 1
  • Definition 4: Stationary Process Invertibility
  • Theorem 2: $\ell^1$ Invertibility Condition
  • Theorem 3: Nagy dilation
  • Proposition 1
  • proof
  • Proposition 2
  • ...and 3 more