In
mathematics, 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 oper ...
, 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 natu ...
. 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
unitary operator
In functional analysis, a unitary operator is a surjective bounded operator on a Hilbert space that preserves the inner product. Unitary operators are usually taken as operating ''on'' a Hilbert space, but the same notion serves to define the c ...
.
In
time series analysis
In mathematics, a time series is a series of data points indexed (or listed or graphed) in time order. Most commonly, a time series is a sequence taken at successive equally spaced points in time. Thus it is a sequence of discrete-time data. ...
, the theorem implies that any
stationary discrete-time
stochastic process can be decomposed into a pair of uncorrelated processes, one deterministic, and the other being a
moving average process.
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
:
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 ''H
α'', 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:
:
where ''V''(''H'') denotes the range of ''V''. The above defined ''H''
''i'' = ''V''
''i''(''H''). If one defines
:
then
:
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 ''M
i'' is isomorphic to another, with ''V'' being an isomorphism between ''M
i'' and ''M''
''i''+1: ''V'' "shifts" ''M
i'' to ''M''
''i''+1. Suppose the dimension of each ''M
i'' 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. T ...
''α''. We see that ''K''
1 can be written as a direct sum Hilbert spaces
:
where each ''H
α'' is an invariant subspaces of ''V'' and ''V'' restricted to each ''H
α'' is the unilateral shift ''S''. Therefore
:
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 color ...
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
:
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 continu ...
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 ''T
z''.
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:
#
#
#The semicommutator
is compact.
The Wold decomposition says that ''V'' is the direct sum of copies of ''T''
''z'' and then some unitary ''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
:
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 ''T
f'' is not compact for any non-zero ''f'' ∈ ''C''(T) and thus ''T
f'' + ''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
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*
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{{Functional analysis
Operator theory
Invariant subspaces
C*-algebras
Theorems in functional analysis
de:Shiftoperator#Wold-Zerlegung