Alphabeta Math
ExampleConstruction: AI-adaptedVerification: AI-adaptedPipeline-generatedaudited 2026-09-22
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Polar decomposition of the unilateral shift

Example

Assume AC. On H=2(N0;C) let S be the unilateral shift Sen=en+1. Then SS=I, SS=IP where P is the orthogonal projection onto Ce0, and S=I; the polar partial isometry of S is S itself, with initial space H and final space (Ce0). In particular S is an isometry that is not a coisometry and not unitary.

Facts & Assumptions

[A1]

2(N0;C) has orthonormal basis (en) with x,en=xn, and every x is the norm limit of its finite expansions n<Nx,enen; the closed linear span of {en:n1} is exactly (Ce0) (Square-summable families on an arbitrary index set and the space 2(I), A Hilbert space with a given orthonormal basis is 2 of the index set, Fourier expansion in a Hilbert space, The Hilbert orthogonal projection onto a closed subspace).

[A2]

Sx,y=x,Sy, so SS and SS are determined by their values on the basis; an isometry is exactly an operator with UU=I, a coisometry has UU=I, 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).

[A3]

S=(SS)1/2 is the unique positive square root, and the polar partial isometry U satisfies S=US and kerU=kerS, with initial space ranS and final space ranS (Absolute value of a bounded operator, Polar decomposition for bounded operators).

[A4]

AC is the hypothesis of the polar-decomposition and Hilbert-space suppliers (The Axiom of Choice).

Verification

technique · direct

Given: The shift S on 2(N0;C) defined by Sen=en+1.

1.1

S is a well-defined bounded linear isometry: for x=nxnen the series Sx=nxnen+1 converges with Sx22=nxn2=x22, so SS=I and S=1.

A1A2
2.1

SS=IP: for the basis vectors Se0=0 and Sen+1=en, so SSem,ek=Sem,Sek equals 1 for m=k1 and 0 otherwise; hence SS is the identity on the closed span of {en:n1}=(Ce0) and vanishes on Ce0.

step 1.1A1A2
2.2

S=I: since SS=I, the identity is positive with square I=SS, so by uniqueness of the positive square root S=I.

step 1.1A3
3.1

Consequently kerS={0} and ranS=(Ce0), and S is an isometry that is not a coisometry: SSI because SSe0=0.

step 1.1step 2.1
4.1

The polar partial isometry of S is U=S: indeed S=SI=SS, kerS={0}=kerU, and S is a partial isometry, being isometric on H=(kerS) and vanishing on kerS={0}; uniqueness in the polar decomposition identifies it.

step 3.1step 2.2A2A3
5.1

The initial space is (kerS)=H and the final space is ranS=(Ce0), as asserted.

step 4.1A4

Depends on

Used by

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Sources