Spectrum of Element of Unital C*-Subalgebra of Unital C*-Algebra
Theorem
Let $\struct {A, \ast, \norm {\, \cdot \,} }$ be a unital $\text C^\ast$-algebra with identity element ${\mathbf 1}_A$.
Let $B \subseteq A$ be a unital $\text C^\ast$-subalgebra of $A$.
Let $\sigma_A$ and $\sigma_B$ be the spectrum in $A$ and $B$ respectively.
Let $x \in B$.
Then we have:
- $\map {\sigma_A} x = \map {\sigma_B} x$
Proof
First take $x$ to be Hermitian.
Let $B' \subseteq B$ be the $\text C^\ast$-algebra generated by $\set { {\mathbf 1}_A, x}$.
By C*-Algebra Generated by Commutative Self-Adjoint Set is Commutative, $B'$ is commutative.
From Spectrum of Hermitian Element in Unital C*-Algebra is Real, we have $\map {\sigma_{B'} } x \subseteq \R$.
From Spectrum of Element in Unital Subalgebra, we therefore have $\map {\sigma_B} x \subseteq \map {\sigma_{B'} } x \subseteq \R$.
From Interior of Set of Real Numbers in Complex Numbers is Empty: Corollary, we have $\map {\sigma_B} x^\circ = \O$ where $\map {\sigma_B} x^\circ$ denotes the interior of $\map {\sigma_B} x$.
From the definition of boundary, we have that $\partial \map {\sigma_B} x = \map {\sigma_B} x^- \setminus \map {\sigma_B} x^\circ$.
Since $\map {\sigma_B} x$ is closed from Spectrum of Element of Banach Algebra is Closed and $\map {\sigma_B} x^\circ = \O$, we then have that $\map {\sigma_B} x = \partial \map {\sigma_B} x$.
Then, from Boundary of Spectrum of Element in Subalgebra of Unital Banach Algebra we have:
- $\map {\sigma_B} x = \partial \map {\sigma_B} x \subseteq \partial \map {\sigma_A} x$
From Set is Closed iff it Contains its Boundary, we have $\partial \map {\sigma_A} x \subseteq \map {\sigma_A} x$.
So $\map {\sigma_B} x \subseteq \map {\sigma_A} x$.
From Spectrum of Element in Unital Subalgebra we have $\map {\sigma_A} x \subseteq \map {\sigma_B} x$.
Hence we conclude $\map {\sigma_A} x = \map {\sigma_B} x$ in this case.
In particular, $0 \in \map {\sigma_A} x$ if and only if $0 \in \map {\sigma_B} x$.
Hence if $x$ is Hermitian, it is invertible in $B$ if and only if it is invertible in $A$.
Let $b \in B$.
Suppose that $b$ is invertible in $A$.
We show that it is invertible in $B$.
Take $a \in A$ such that $a b = b a = {\mathbf 1}_A$.
From Inverse of Star of Element in Unital *-Algebra, we have $b^\ast a^\ast = a^\ast b^\ast = {\mathbf 1}_A$.
We therefore have:
\(\ds b b^\ast a^\ast a\) | \(=\) | \(\ds b \paren {b^\ast a^\ast} a\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds b {\mathbf 1}_A a\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds b a\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds {\mathbf 1}_A\) |
and:
\(\ds a^\ast a b b^\ast\) | \(=\) | \(\ds a^\ast \paren {a b} b^\ast\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds a^\ast {\mathbf 1}_A b^\ast\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds a^\ast b^\ast\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds {\mathbf 1}_A\) |
Hence $b b^\ast$ is invertible in $A$.
From Product of Element in *-Star Algebra with its Star is Hermitian, $b b^\ast$ is Hermitian.
Hence from what we have already shown, $b b^\ast$ is invertible in $B$.
So there exists $c \in B$ such that $b b^\ast c = {\mathbf 1}_A$.
Then:
\(\ds a\) | \(=\) | \(\ds a b b^\ast c\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \paren {a b} b^\ast c\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds {\mathbf 1}_A b^\ast c\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds b^\ast c\) |
Since $b^\ast \in B$ and $c \in B$, we have $a \in B$.
So $b$ is invertible in $B$.
Clearly conversely if $b$ is invertible in $B$, then it is invertible in $A$.
Hence we have shown that if $b \in B$, then $b$ is invertible in $B$ if and only if it is invertible in $A$.
In particular, if $x \in B$ then ${\mathbf 1}_A - x$ is invertible in $B$ if and only if it is invertible in $A$.
This is precisely the statement $\map {\sigma_A} x = \map {\sigma_B} x$.
$\blacksquare$
Sources
- 1990: Gerard J. Murphy: C*-Algebras and Operator Theory ... (previous) ... (next): $2.1.11$: Theorem