Beurling's theorem on shift-invariant subspaces

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The commutant of the unilateral shift is the set of all restrictions to H2\mathbf{H}^2 of multiplications by multipliers in H∞\mathbf{H}^{\infty }.

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Remark.
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The commutant of an operator (or of a set of operators) is the set of all operators that commute with it (or with each operator in the set). The unilateral shift is the restriction of the bilateral shift WW to H2\mathbf{H}^2, where H2\mathbf{H}^2 is the closed span in L2L^2 of the unit circle of the functions ene_n, n=0,1,2,…n = 0, 1, 2, \ldots (with en(z)=zne_n(z) = z^n), and H∞\mathbf{H}^{\infty } is the set of essentially bounded functions in H2\mathbf{H}^2. If the bilateral shift is regarded as a multiplication (by e1e_1 on L2L^2), then its commutant is the set of all multiplications on the same L2L^2 (Problem 146). If, however, the multiplier itself is in H2\mathbf{H}^2 (and hence in H∞\mathbf{H}^{\infty }), then H2\mathbf{H}^2 is invariant under the induced multiplication (cf. Problem 34), and the restriction of that multiplication to H2\mathbf{H}^2 makes sense.

If UU is the (simple) unilateral shift and if M\mathbf{M} is a non-zero subspace invariant under UU, then there exists a (necessarily unique) one-dimensional wandering subspace N\mathbf{N} such that M=⋁n=0∞UnN\mathbf{M} = \bigvee_{n=0}^{\infty } U^n \mathbf{N}.

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Remark.
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If AA is an operator on a Hilbert space H\mathbf{H}, a subspace N\mathbf{N} of H\mathbf{H} is called wandering for AA if it is orthogonal to all its images under the positive powers of AA.

A non-zero subspace M\mathbf{M} of H2\mathbf{H}^2 is invariant under UU if and only if there exists a function φ\varphi in H∞\mathbf{H}^{\infty }, of constant modulus 11 almost everywhere, such that M\mathbf{M} is the range of the restriction to H2\mathbf{H}^2 of the multiplication induced by φ\varphi.

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Remark.
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Regard UU as the restriction to H2\mathbf{H}^2 of the multiplication induced by e1e_1 on L2L^2 of the unit circle. A function φ\varphi in H∞\mathbf{H}^{\infty } of constant modulus 11 almost everywhere is called an inner function; informally, M=φ⋅H2\mathbf{M} = \varphi \cdot \mathbf{H}^2 can be described as the set of all multiples of φ\varphi by functions in H2\mathbf{H}^2.

Find the conditions mentioned in Sec. 17.22.

Section 17.22 (Remark): Let SS be the shift operator on H2H^{2}, (Sf)(z)=zf(z)(S f)(z) = z f(z) (f∈H2,z∈U)(f \in H^{2}, z \in U); a closed subspace YY of H2H^{2} with S(Y)⊂YS(Y) \subset Y is called SS-invariant. By Beurling's theorem (Theorem 17.21), every closed SS-invariant subspace of H2H^{2} other than {0}\left\{ 0\right\} is of the form φH2={φf:f∈H2}\varphi H^{2} = \left\{ \varphi f: f \in H^{2}\right\} for an inner function φ\varphi, and φ\varphi is determined by the subspace up to a constant factor; by Theorem 17.15, every inner function has the form

M(z)=cB(z)exp⁡{−∫−ππeit+zeit−zdμ(t)}(z∈U), M(z) = c B(z) \exp \left\{ -\int _{-\pi }^{\pi } \frac{e^{i t}+z}{e^{i t}-z} d \mu (t)\right\} \quad (z \in U),

where cc is a constant, ∣c∣=1\left|c\right| = 1, BB is a Blaschke product, and μ\mu is a finite positive Borel measure on TT which is singular with respect to Lebesgue measure. Combining these, the SS-invariant subspaces of H2H^{2} are characterized by the following data: a sequence of complex numbers {αn}\left\{ \alpha_{n}\right\} (possibly finite, or even empty) such that ∣αn∣<1\left|\alpha_{n}\right| < 1 and Σ(1−∣αn∣)<∞\Sigma \left(1-\left|\alpha_{n}\right|\right) < \infty (the zeros of BB), and a positive Borel measure μ\mu on TT, singular with respect to Lebesgue measure. The book states that it is easy to find conditions, in terms of {αn}\left\{ \alpha_{n}\right\} and μ\mu, which ensure that one SS-invariant subspace of H2H^{2} contains another.

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References

[Hal82] Halmos P.R. A Hilbert Space Problem Book. 2nd ed., Springer-Verlag, 1982.
[Rud87] Rudin W. Real and Complex Analysis. 3rd ed., McGraw-Hill, 1987.