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Wold's decomposition

In mathematics, particularly in operator theory, Wold decomposition or Wold–von Neumann decomposition, named after Herman Wold and John von Neumann, is a classification theorem for isometric linear operators on a given Hilbert space. It states that every isometry is a direct sum of copies of the unilateral shift and a unitary operator.

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Let H be a Hilbert space, L(H) be the bounded operators on H, and VL(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 , 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 is an invariant subspaces of V and V restricted to each 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 ==
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 ==
The C*-algebra generated by an isometry
Consider an isometry VL(H). Denote by C*(V) the C*-algebra 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) = {Tf + K | Tf is a Toeplitz operator with continuous symbol fC(T) and K is a compact operator}. In this identification, S = Tz 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_{f+g}.\, • T_f ^* = T_ . • The semicommutator T_fT_g - T_{fg} \, is compact. The Wold decomposition says that V is the direct sum of copies of Tz and then some unitary U: :V = \left( \bigoplus_{\alpha \in A} T_z \right) \oplus U. So we invoke the continuous functional calculus ff(U), and define : \Phi : C^*(S) \rightarrow C^*(V) \quad \text{by} \quad \Phi(T_f + K) = \bigoplus_{\alpha \in A} (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 fC(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 ==
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