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ExampleConstruction: Literature-sourcedVerification: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-22
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Adjoint, norm and trace of an operator of rank at most one

Example

Assume the Axiom of Countable Choice (The Axiom of Countable Choice (ACω)). Let H be a real or complex Hilbert space with the pairing linear in the first argument (Hilbert space, Real and complex inner-product spaces and their induced length), let u,vH and let T:=Tu,vB(H),Tx:=x,vu. Then:

  1. the Hilbert adjoint is Tx=x,uv (The Hilbert-space adjoint of a bounded operator, Hilbert-adjoint identities);
  2. T=uv (The operator norm as the least bound and as the unit-sphere or unit-ball supremum);
  3. T is trace class (Trace class operator); if u0 and v0 its singular values are s1(T)=uv and sn(T)=0 for n2, so it has exactly one nonzero singular value, and T1=uv; if u=0 or v=0 then T=0 and all singular values vanish;
  4. tr(T)=u,v (Trace is absolutely convergent and basis independent).

Facts & Assumptions

Given: Countable Choice, the Hilbert space H, vectors u,vH and the operator of rank at most one T=,vu.

[A1]

Pairing and adjoint. The pairing is linear in the first argument, conjugate-linear in the second, conjugate symmetric with w,w=w20; the Hilbert adjoint is characterised by Tx,y=x,Ty and satisfies T=T, (ST)=TS (Real and complex inner-product spaces and their induced length, The Hilbert-space adjoint of a bounded operator, Hilbert-adjoint identities, Hilbert space).

[A3]

Compactness and spectral data. Every bounded finite-rank operator is compact (Bounded finite rank operators are compact). A nonzero compact self-adjoint positive operator has a largest eigenvalue equal to its norm with unit eigenvector, its nonzero eigenvalues are positive with finite multiplicities accumulating only at 0, its closed span is (ker), and the positive square root is unique; the singular values of a compact operator are the positive eigenvalues of T with multiplicity, in nonincreasing order with zero padding (Norm point of a compact self adjoint operator is an eigenvalue up to sign, Spectral theorem for compact self adjoint operators, Positive square root of a compact positive operator, Absolute value and singular values of a compact operator, Singular value decomposition for compact operators).

[A4]

Trace machinery. A compact operator with nsn<+ is trace class with T1=nsn; for a nuclear representation T=j,ujvj the trace is jvj,uj, independently of the representation, and tr(T)T1 (Trace class operator, Nuclear series characterizes trace norm, Trace is absolutely convergent and basis independent, Trace of a trace class operator).

Verification

technique · direct

Given: Countable Choice, the vectors u,v, the operator T=,vu, and the candidate T:=,uv.

1.1

The adjoint. The candidate is linear by first-variable linearity and bounded by x,uvuvx using [A2]. For all x,yH, Tx,y=x,vu,y=x,vu,y and x,Ty=x,y,uv=y,ux,v=u,yx,v by conjugate symmetry [A1]; the two expressions agree, so by uniqueness of the Hilbert adjoint T=,uv.

A1A2
1.2

The norm. For every x, Tx=x,vuuvx by [A2], so Tuv; if v0 then testing x=v/v gives Tx=vu, whence equality, and if v=0 then T=0 and both sides are 0.

A1A2algebra
2.1

The singular value. The range of T is contained in span{u}, when u,v0, T(v/v2)=u, so its range has ordered basis (u); if either vector is zero its range has the empty basis. Thus the bounded operator T has finite rank and is compact by [A3]. Compute TTx=x,vu2v using [step 1.1] and conjugate linearity in the second argument [A1]; hence TT=u2v2P where P:=,v/vv/v is the orthogonal projection onto span{v} when v0, and put P=0 when v=0, so the displayed formula holds in that case too. For v0, writing e=v/v gives P2=P, P=P and Px,x=x,e20 directly from [A1]. The operator S:=uvP is bounded by [A2] and has the one-vector range basis (v) when u,v0, otherwise the empty range basis. It is therefore compact by [A3], and is self-adjoint and positive with S2=TT, so T=S by uniqueness of the positive square root [A3]; its nonzero eigenvalues are the single number uv with multiplicity one when u,v0, and there are none when u=0 or v=0. By [A3] the singular values of T are exactly this data, and [A4] gives T1=uv<+, so T is trace class.

step 1.1A1A2A3A4algebra
3.1

The trace. Assume u,v0 (otherwise T=0 and the trace is 0=u,v). Then, writing e:=v/v and s:=uv, the identity Tx=sx,e(u/u) exhibits T as the positive-integer-indexed nuclear representation with u1:=e, v1:=su/u=vu and uj=vj=0 for j2. Its zero-based partial-sum sequence has R0=0 and Rm=T for every m1, so it converges to T exactly as required by [A4]. Therefore tr(T)=v1,u1=vu,v/v=u,v, since scalar multiplication in the first argument and conjugate-linearity in the second give vu,v/v=vv1u,v=u,v.

step 2.1A1A4algebra
4.1

Conclusion. Claims 1–4 are [step 1.1], [step 1.2], [step 2.1] and [step 3.1]; in the degenerate cases u=0 or v=0 the operator is 0 with T=T1=0 and tr(T)=0=u,v.

step 1.1step 1.2step 2.1step 3.1

Depends on

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Dependency tree · two levels

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