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 = \left(\bigoplus_{\alpha \in A} S\right) \oplus U for some index set
A, where
S is the
unilateral shift on a Hilbert space
Hα, and
U is a unitary operator (possible vacuous). The family {
Hα} 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
Hi =
Vi(
H). If one defines :M_i = H_i \ominus H_{i+1} = V^i (H \ominus V(H)) \quad \text{for} \quad i \geq 0 \;, then :H = \left( \bigoplus_{i \geq 0} M_i \right) \oplus \left( \bigcap_{i \geq 0} H_i \right) = K_1 \oplus K_2. It is clear that
K1 and
K2 are invariant subspaces of
V. So
V(
K2) =
K2. In other words,
V restricted to
K2 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
Mi+1:
V "shifts"
Mi to
Mi+1. Suppose the dimension of each
Mi is some
cardinal number α. We see that
K1 can be written as a direct sum Hilbert spaces :K_1 = \oplus H_{\alpha} where each
Hα is an invariant subspaces of
V and
V restricted to each
Hα is the unilateral shift
S. Therefore :V = V \vert_{K_1} \oplus V\vert_{K_2} = \left(\bigoplus_{\alpha \in A} S \right) \oplus U, which is a Wold decomposition of
V.
Remarks It is immediate from the Wold decomposition that the
spectrum 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, \bigcap_{i\ge0} H_i = \{0\}. 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 = \bigoplus_{1 \le \alpha \le N} 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
Vn(
M) ⊥
Vm(
M) for all
n ≠
m. In particular, each
Mi defined above is a wandering subspace of
V. == A sequence of isometries ==