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Spectral permanence for unital c star subalgebras

Statement

Assume AC. If B is a unital C*-subalgebra of a unital C*-algebra A with the same identity, then σB(b)=σA(b) for every bB.

Facts & Assumptions

[A1]

A unital C*-algebra is a nonzero complex Banach algebra with a unit of norm one and an involution satisfying the C*-identity; a unital C*-subalgebra with the same identity is a closed unital -subalgebra containing that unit (C star algebra, Unital Banach algebra).

[A2]

For every element b invertible in A the adjoint b is invertible with (b)1=(b1), and bb is positive; positivity of an element means x=yy for some element y (Self-adjoint positive unitary and normal elements for positivity, C star algebra for the involution rules).

[A3]

If BA is a unital subalgebra with the same unit and bB, then σA(b)σB(b), since invertibility in B implies invertibility in A (Spectrum and resolvent set in a Banach algebra).

[A4]

For a nonzero unital commutative complex C*-algebra C the Gelfand transform Γ:CC(Δ(C)) is an isometric unital -isomorphism onto C(Δ(C)), and Δ(C) is a nonempty compact Hausdorff space (Commutative Gelfand Naimark, Maximal ideal space is compact Hausdorff, Character and maximal ideal space).

[A5]

A unital self-adjoint complex function algebra that separates the points of a nonempty compact Hausdorff space is uniformly dense in all continuous complex functions (Complex Stone–Weierstrass dichotomy for separating self-adjoint algebras; the unital case is dense).

[A6]

Characters of a unital commutative complex C*-algebra satisfy χ(c)=χ(c) (Characters on a unital commutative C star algebra preserve star).

[A7]

AC is the global hypothesis of the Gelfand-theoretic suppliers (The Axiom of Choice).

Proof

technique · direct

Given: A unital C*-algebra A, a unital C*-subalgebra BA with 1B=1A, and bB.

1.1

Since invertibility in B implies invertibility in A, one has σA(b)σB(b); it remains to prove the reverse inclusion, that is, that b invertible in A is invertible in B with inverse in B.

A3
1.2

If b is invertible in A, then x:=bbB is positive and invertible in A with x1=b1(b1); and if x positive and invertible in A has x1B, then (bb)1B and b1=(bb)1bB.

A1A2algebra
1.3

It suffices to treat a self-adjoint xB invertible in A, because the positive element bb in the preceding reduction is self-adjoint. For such x, let C:=CA(1,x,x1) be the closed unital star-subalgebra of A generated by x and x1, and let D:=CA(1,x)B. Both are commutative, because x=x and (x1)=x1, and the Gelfand transform is an isometric unital star-isomorphism Γ:CC(Δ(C)) on the nonempty compact Hausdorff character space.

A1A2A4A7algebra
2.1

The function x^ separates the points of Δ(C). Indeed, if characters h,h have h(x)=h(x), then h(x1)=h(x)1=h(x)1=h(x1); they therefore agree on the unital star-algebra generated by x,x1 and, by continuity, on its closure C, so h=h. Moreover x^ is real-valued because x=x and characters preserve the involution.

step 1.3A6algebra
3.1

Under Γ, the algebra D is the closed unital self-adjoint function algebra generated by x^. It separates points by step 2.1, so Stone--Weierstrass gives Γ(D)=C(Δ(C))=Γ(C). Injectivity of Γ yields D=C, hence x1DB.

step 2.1A4A5
4.1

Therefore every bB invertible in A has (bb)1B by step 3.1 and then b1=(bb)1bB by step 1.2. Thus σB(b)σA(b); with step 1.1 this gives σB(b)=σA(b).

step 1.1step 1.2step 3.1

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