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Polar decomposition of the unilateral shift
Example
Assume AC. On let be the unilateral shift . Then , where is the orthogonal projection onto , and ; the polar partial isometry of is itself, with initial space and final space . In particular is an isometry that is not a coisometry and not unitary.
Facts & Assumptions
has orthonormal basis with , and every is the norm limit of its finite expansions ; the closed linear span of is exactly (Square-summable families on an arbitrary index set and the space , A Hilbert space with a given orthonormal basis is of the index set, Fourier expansion in a Hilbert space, The Hilbert orthogonal projection onto a closed subspace).
, so and are determined by their values on the basis; an isometry is exactly an operator with , a coisometry has , and a partial isometry vanishes on its kernel and is isometric on the orthogonal complement of the kernel (Hilbert-adjoint identities, Isometry coisometry and partial isometry).
is the unique positive square root, and the polar partial isometry satisfies and , with initial space and final space (Absolute value of a bounded operator, Polar decomposition for bounded operators).
AC is the hypothesis of the polar-decomposition and Hilbert-space suppliers (The Axiom of Choice).
Verification
Given: The shift on defined by .
is a well-defined bounded linear isometry: for the series converges with , so and .
: for the basis vectors and , so equals for and otherwise; hence is the identity on the closed span of and vanishes on .
: since , the identity is positive with square , so by uniqueness of the positive square root .
Consequently and , and is an isometry that is not a coisometry: because .
The polar partial isometry of is : indeed , , and is a partial isometry, being isometric on and vanishing on ; uniqueness in the polar decomposition identifies it.
The initial space is and the final space is , as asserted.
Depends on
- Polar decomposition for bounded operators
- The Axiom of Choice
- Square-summable families on an arbitrary index set and the space $\ell^2(I)$
- A Hilbert space with a given orthonormal basis is $\ell^2$ of the index set
- Isometry coisometry and partial isometry
- Fourier expansion in a Hilbert space
- Orthogonality and the orthogonal complement
- The Hilbert orthogonal projection onto a closed subspace
- Absolute value of a bounded operator
- Hilbert-adjoint identities
Used by
Nothing in the library uses this result yet.
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Sources
- John B. Conway, A Course in Functional Analysis, 2nd ed., Chapter IX §3, printed pp.239–243 (standard reference, not scraped)
- Theo Bühler and Dietmar Salamon, Functional Analysis, §5.3, printed pp.235–245 (standard reference, not scraped)