Wold Decomposition
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, particularly in
operator theory In mathematics, operator theory is the study of linear operators on function spaces, beginning with differential operators and integral operators. The operators may be presented abstractly by their characteristics, such as bounded linear operat ...
, Wold decomposition or Wold–von Neumann decomposition, named after Herman Wold and
John von Neumann John von Neumann (; hu, Neumann János Lajos, ; December 28, 1903 – February 8, 1957) was a Hungarian-American mathematician, physicist, computer scientist, engineer and polymath. He was regarded as having perhaps the widest cove ...
, is a classification theorem for isometric linear operators on a given
Hilbert space In mathematics, Hilbert spaces (named after David Hilbert) allow generalizing the methods of linear algebra and calculus from (finite-dimensional) Euclidean vector spaces to spaces that may be infinite-dimensional. Hilbert spaces arise natural ...
. It states that every isometry is a direct sum of copies of the
unilateral shift In mathematics, and in particular functional analysis, the shift operator also known as translation operator is an operator that takes a function to its translation . In time series analysis, the shift operator is called the lag operator. Shift ...
and a
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. In
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, the theorem implies that any stationary discrete-time
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can be decomposed into a pair of uncorrelated processes, one deterministic, and the other being a
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.


Details

Let ''H'' be a Hilbert space, ''L''(''H'') be the bounded operators on ''H'', and ''V'' ∈ ''L''(''H'') be an isometry. The Wold decomposition states that every isometry ''V'' takes the form :V = (\oplus_ S) \oplus U for some index set ''A'', where ''S'' is the
unilateral shift In mathematics, and in particular functional analysis, the shift operator also known as translation operator is an operator that takes a function to its translation . In time series analysis, the shift operator is called the lag operator. Shift ...
on a Hilbert space ''Hα'', and ''U'' is a unitary operator (possible vacuous). The family consists of isomorphic Hilbert spaces. A proof can be sketched as follows. Successive applications of ''V'' give a descending sequences of copies of ''H'' isomorphically embedded in itself: :H = H \supset V(H) \supset V^2 (H) \supset \cdots = H_0 \supset H_1 \supset H_2 \supset \cdots, where ''V''(''H'') denotes the range of ''V''. The above defined ''H''''i'' = ''V''''i''(''H''). If one defines :M_i = H_i \ominus H_ = V^i (H \ominus V(H)) \quad \text \quad i \geq 0 \;, then :H = (\oplus_ M_i) \oplus (\cap_ H_i) = K_1 \oplus K_2. It is clear that ''K''1 and ''K''2 are invariant subspaces of ''V''. So ''V''(''K''2) = ''K''2. In other words, ''V'' restricted to ''K''2 is a surjective isometry, i.e., a unitary operator ''U''. Furthermore, each ''Mi'' is isomorphic to another, with ''V'' being an isomorphism between ''Mi'' and ''M''''i''+1: ''V'' "shifts" ''Mi'' to ''M''''i''+1. Suppose the dimension of each ''Mi'' is some
cardinal number In mathematics, cardinal numbers, or cardinals for short, are a generalization of the natural numbers used to measure the cardinality (size) of sets. The cardinality of a finite set is a natural number: the number of elements in the set. Th ...
''α''. We see that ''K''1 can be written as a direct sum Hilbert spaces :K_1 = \oplus H_ where each ''Hα'' is an invariant subspaces of ''V'' and ''V'' restricted to each ''Hα'' is the unilateral shift ''S''. Therefore :V = V \vert_ \oplus V\vert_ = (\oplus_ S) \oplus U, which is a Wold decomposition of ''V''.


Remarks

It is immediate from the Wold decomposition that the
spectrum A spectrum (plural ''spectra'' or ''spectrums'') is a condition that is not limited to a specific set of values but can vary, without gaps, across a continuum. The word was first used scientifically in optics to describe the rainbow of colors i ...
of any proper, i.e. non-unitary, isometry is the unit disk in the complex plane. An isometry ''V'' is said to be pure if, in the notation of the above proof, ∩''i''≥0 ''H''''i'' = . The multiplicity of a pure isometry ''V'' is the dimension of the kernel of ''V*'', i.e. the cardinality of the index set ''A'' in the Wold decomposition of ''V''. In other words, a pure isometry of multiplicity ''N'' takes the form :V = \oplus_ S . In this terminology, the Wold decomposition expresses an isometry as a direct sum of a pure isometry and a unitary operator. A subspace ''M'' is called a wandering subspace of ''V'' if ''V''''n''(''M'') ⊥ ''V''''m''(''M'') for all ''n'' ≠ ''m''. In particular, each ''M''''i'' defined above is a wandering subspace of ''V''.


A sequence of isometries

The decomposition above can be generalized slightly to a sequence of isometries, indexed by the integers.


The C*-algebra generated by an isometry

Consider an isometry ''V'' ∈ ''L''(''H''). Denote by ''C*''(''V'') the
C*-algebra In mathematics, specifically in functional analysis, a C∗-algebra (pronounced "C-star") is a Banach algebra together with an involution satisfying the properties of the adjoint. A particular case is that of a complex algebra ''A'' of continuous ...
generated by ''V'', i.e. ''C*''(''V'') is the norm closure of polynomials in ''V'' and ''V*''. The Wold decomposition can be applied to characterize ''C*''(''V''). Let ''C''(T) be the continuous functions on the unit circle T. We recall that the C*-algebra ''C*''(''S'') generated by the unilateral shift ''S'' takes the following form :''C*''(''S'') = . In this identification, ''S'' = ''T''''z'' where ''z'' is the identity function in ''C''(T). The algebra ''C*''(''S'') is called the Toeplitz algebra. Theorem (Coburn) ''C*''(''V'') is isomorphic to the Toeplitz algebra and ''V'' is the isomorphic image of ''Tz''. The proof hinges on the connections with ''C''(T), in the description of the Toeplitz algebra and that the spectrum of a unitary operator is contained in the circle T. The following properties of the Toeplitz algebra will be needed: #T_f + T_g = T_.\, # T_f ^* = T_ . #The semicommutator T_fT_g - T_ \, is compact. The Wold decomposition says that ''V'' is the direct sum of copies of ''T''''z'' and then some unitary ''U'': :V = (\oplus_ T_z) \oplus U. So we invoke the
continuous functional calculus In mathematics, particularly in operator theory and C*-algebra theory, a continuous functional calculus is a functional calculus which allows the application of a continuous function to normal elements of a C*-algebra. Theorem Theorem. Let ' ...
''f'' → ''f''(''U''), and define : \Phi : C^*(S) \rightarrow C^*(V) \quad \text \quad \Phi(T_f + K) = \oplus_ (T_f + K) \oplus f(U). One can now verify Φ is an isomorphism that maps the unilateral shift to ''V'': By property 1 above, Φ is linear. The map Φ is injective because ''Tf'' is not compact for any non-zero ''f'' ∈ ''C''(T) and thus ''Tf'' + ''K'' = 0 implies ''f'' = 0. Since the range of Φ is a C*-algebra, Φ is surjective by the minimality of ''C*''(''V''). Property 2 and the continuous functional calculus ensure that Φ preserves the *-operation. Finally, the semicommutator property shows that Φ is multiplicative. Therefore the theorem holds.


References

* * * * {{Functional analysis Operator theory Invariant subspaces C*-algebras Theorems in functional analysis de:Shiftoperator#Wold-Zerlegung