🎵C*-algebras Unit 9 – Spectral Theory in C*–algebras
Spectral theory in C*-algebras explores the properties of spectra, which are sets of complex numbers associated with elements in these algebras. This theory provides powerful tools for understanding the structure of C*-algebras and their elements, including normal operators, self-adjoint operators, and unitary operators.
Key concepts include the spectrum, resolvent set, and spectral radius. Important results like the Spectral Theorem and Gelfand-Naimark Theorem form the foundation of this theory. The continuous functional calculus and spectral mapping theorem are essential tools for working with functions of operators in C*-algebras.
C*-algebra a complex Banach algebra with an involution satisfying the C*-identity ∥a∗a∥=∥a∥2
Spectrum of an element a in a C*-algebra A, denoted by σ(a), the set of all λ∈C such that a−λ1 is not invertible in A
Resolvent set of an element a in a C*-algebra A, the complement of the spectrum, i.e., all λ∈C such that a−λ1 is invertible in A
Resolvent function R(λ,a)=(a−λ1)−1 for λ in the resolvent set of a
Point spectrum of an element a, the set of all eigenvalues of a, i.e., all λ∈C such that a−λ1 is not injective
Continuous spectrum of an element a, the set of all λ∈σ(a) that are not eigenvalues and for which a−λ1 is not surjective
Residual spectrum of an element a, the set of all λ∈σ(a) that are not eigenvalues and for which a−λ1 is not injective
Spectral radius of an element a, denoted by r(a), the radius of the smallest closed disk centered at the origin containing σ(a), i.e., r(a)=sup{∣λ∣:λ∈σ(a)}
Fundamental Theorems
Spectral Theorem for Normal Elements if a is a normal element in a C*-algebra A, then there exists a unique *-homomorphism Φ:C(σ(a))→C∗(a) such that Φ(id)=a, where id is the identity function on σ(a)
Consequence every normal element in a C*-algebra can be represented as a continuous function on its spectrum
Spectral Theorem for Commutative C*-algebras every commutative C*-algebra A is *-isomorphic to C(X) for some compact Hausdorff space X
X is homeomorphic to the space of characters (non-zero *-homomorphisms) on A
Gelfand-Naimark Theorem every C*-algebra A can be isometrically *-isomorphically embedded into B(H) for some Hilbert space H
Consequence C*-algebras can be concretely represented as norm-closed *-subalgebras of bounded operators on a Hilbert space
Functional Calculus Theorem for any normal element a in a C*-algebra A and any continuous function f on σ(a), there exists a unique element f(a) in C∗(a) such that Φ(f)=f(a), where Φ is the *-homomorphism from the Spectral Theorem
Spectral Permanence Theorem if ϕ:A→B is a -homomorphism between C-algebras and a∈A, then σ(ϕ(a))∪{0}=ϕ(σ(a))∪{0}
Consequence *-homomorphisms preserve spectra up to the possible addition of 0
Spectral Properties of Operators
Spectrum of a self-adjoint operator is real, i.e., if a=a∗, then σ(a)⊆R
Spectrum of a unitary operator lies on the unit circle, i.e., if u∗u=uu∗=1, then σ(u)⊆{z∈C:∣z∣=1}
Spectrum of a positive operator is non-negative, i.e., if a≥0, then σ(a)⊆[0,∞)
An element a is positive if a=b∗b for some b in the C*-algebra
Spectral radius formula r(a)=limn→∞∥an∥1/n for any element a in a C*-algebra
Spectrum of a normal operator is contained in the numerical range, i.e., if a is normal, then σ(a)⊆{(ax,x):x∈H,∥x∥=1}, where H is the Hilbert space on which a acts
Compact operators have discrete spectrum, i.e., if a is compact, then σ(a)∖{0} consists only of eigenvalues with finite multiplicities
Multiplicities of eigenvalues are the dimensions of the corresponding eigenspaces
Continuous Functional Calculus
Continuous Functional Calculus for any normal element a in a C*-algebra A, there is a *-homomorphism Φ:C(σ(a))→C∗(a) such that Φ(id)=a, where id is the identity function on σ(a)
Allows for the definition of f(a) for any continuous function f on σ(a)
Properties of the functional calculus
Φ is a unital *-homomorphism, i.e., Φ(1)=1 and Φ(f∗)=Φ(f)∗
Φ is norm-decreasing, i.e., ∥Φ(f)∥≤∥f∥∞, where ∥f∥∞ is the supremum norm of f on σ(a)
Φ is spectrum-preserving, i.e., σ(Φ(f))=f(σ(a)) for any continuous function f on σ(a)
Holomorphic functional calculus an extension of the continuous functional calculus to holomorphic functions on a neighborhood of σ(a)
Allows for the definition of f(a) for holomorphic functions f, not just continuous functions
Borel functional calculus a further extension to bounded Borel functions on σ(a)
Requires the use of spectral measures and integration theory
Spectral Mapping Theorem
Spectral Mapping Theorem for any normal element a in a C*-algebra A and any continuous function f on σ(a), we have σ(f(a))=f(σ(a))
Consequence the spectrum of f(a) is the image of the spectrum of a under the function f
Examples
If a is self-adjoint and f(t)=t2, then σ(a2)={λ2:λ∈σ(a)}
If u is unitary and f(z)=zn for some integer n, then σ(un)={zn:z∈σ(u)}
Spectral Mapping Theorem for holomorphic functions if f is holomorphic on a neighborhood of σ(a), then σ(f(a))=f(σ(a)), where f(a) is defined using the holomorphic functional calculus
Spectral Mapping Theorem for Borel functions if f is a bounded Borel function on σ(a), then σ(f(a))=f(σ(a)), where f(a) is defined using the Borel functional calculus
Requires more advanced techniques from spectral theory and measure theory
Applications to C*-algebras
Characterization of commutative C*-algebras a C*-algebra A is commutative if and only if it is *-isomorphic to C(X) for some compact Hausdorff space X
X is uniquely determined up to homeomorphism by A
Characterization of -homomorphisms between commutative C-algebras if A and B are commutative C*-algebras, then *-homomorphisms from A to B correspond bijectively to continuous functions from the character space of B to the character space of A
Functional calculus in C*-algebras the continuous functional calculus allows for the definition of f(a) for any normal element a in a C*-algebra A and any continuous function f on σ(a)
Useful for constructing new elements in C*-algebras with desired properties
Spectral permanence in C*-algebras -homomorphisms between C-algebras preserve spectra, i.e., if ϕ:A→B is a *-homomorphism and a∈A, then σ(ϕ(a))∪{0}=ϕ(σ(a))∪{0}
Useful for studying the behavior of spectra under mappings between C*-algebras
Ideal structure of C*-algebras closed two-sided ideals in a C*-algebra A correspond bijectively to open subsets of the primitive ideal space of A
Primitive ideal space consists of kernels of irreducible *-representations of A
Examples and Counterexamples
Example commutative C*-algebras C(X) for compact Hausdorff spaces X
Spectrum of f∈C(X) is the range of f, i.e., σ(f)=f(X)
Example non-commutative C*-algebras B(H) for Hilbert spaces H, Mn(C) for n≥2
Spectrum of an operator T∈B(H) is not always equal to the range of T
Example normal operators self-adjoint operators, unitary operators, projection operators
Spectral theorem applies to these operators
Example non-normal operators shift operator on ℓ2(N), nilpotent operators
Spectral theorem does not apply to these operators
Counterexample spectrum is not always real even for self-adjoint elements in non-commutative C*-algebras
Consider a non-normal element a with a=a∗ in a non-commutative C*-algebra
Counterexample spectrum is not always non-negative even for positive elements in non-commutative C*-algebras
Consider a non-normal positive element a in a non-commutative C*-algebra
Common Pitfalls and Misconceptions
Misconception the spectrum of an element in a C*-algebra is always a subset of R or C
The spectrum can be empty or unbounded in general
Pitfall assuming the spectral theorem holds for all elements in a C*-algebra
The spectral theorem only applies to normal elements
Misconception the spectrum of a self-adjoint element is always real
This is true in commutative C*-algebras but not necessarily in non-commutative C*-algebras
Pitfall confusing the spectrum of an element with its numerical range
The numerical range contains the spectrum but can be strictly larger
Misconception the functional calculus always produces a normal element
The functional calculus preserves normality, but f(a) may not be normal if f is not continuous or if a is not normal