Continuous functional calculus explained

In mathematics, particularly in operator theory and C*-algebra theory, the continuous functional calculus is a functional calculus which allows the application of a continuous function to normal elements of a C*-algebra.

In advanced theory, the applications of this functional calculus are so natural that they are often not even mentioned. It is no overstatement to say that the continuous functional calculus makes the difference between C*-algebras and general Banach algebras, in which only a holomorphic functional calculus exists.

Motivation

\sigma(a) of an element a of a Banach algebra l{A} to a functional calculus for continuous functions C(\sigma(a)) on the spectrum, it seems obvious to approximate a continuous function by polynomials according to the Stone-Weierstrass theorem, to insert the element into these polynomials and to show that this sequence of elements converges to The continuous functions on \sigma(a) \subset \C are approximated by polynomials in z and \overline{z} , i.e. by polynomials of the form Here, \overline{z} denotes the complex conjugation, which is an involution on the To be able to insert a in place of z in this kind of polynomial, Banach *-algebras are considered, i.e. Banach algebras that also have an involution *, and a ^{*} is inserted in place of In order to obtain a homomorphism { C}[z,\overline{z}] → l{A} , a restriction to normal elements, i.e. elements with a ^{*a} = aa ^{*} , is necessary, as the polynomial ring \C[z,\overline{z}] is commutative.If (p _{n(z,\overline{z}))} _{n} is a sequence of polynomials that converges uniformly on \sigma(a) to a continuous function f , the convergence of the sequence (p ^{*))} _{n} in l{A} to an element f(a) must be ensured. A detailed analysis of this convergence problem shows that it is necessary to resort to C*-algebras. These considerations lead to the so-called continuous functional calculus.

Theorem

Due to the *-homomorphism property, the following calculation rules apply to all functions

f,g \in C(\sigma(a)) and scalars λ ,\mu \in \C :

( λ f + \mu g)(a) = λ f(a) + \mu g(a)	(linear)
(f ⋅ g)(a) = f (a) ⋅ g(a)	(multiplicative)
\overline{f}(a) = \colon (f ^{*)(a)} = (f(a)) ^{*}	(involutive)

One can therefore imagine actually inserting the normal elements into continuous functions; the obvious algebraic operations behave as expected.

The requirement for a unit element is not a significant restriction. If necessary, a unit element can be adjoined, yielding the enlarged C*-algebra Then if

a \in l{A} and f \in C(\sigma (a)) with f( 0 ) = 0 , it follows that 0 \in \sigma (a) and

The existence and uniqueness of the continuous functional calculus are proven separately:

• Existence: Since the spectrum of

a in the C*-subalgebra C ^{*(a,e)} generated by a and e is the same as it is in l{A} , it suffices to show the statement for The actual construction is almost immediate from the Gelfand representation: it suffices to assume l{A} is the C*-algebra of continuous functions on some compact space X and define

• Uniqueness: Since

\Phi _{a(\boldsymbol{1})} and \Phi _{a(\operatorname{Id}} _{\sigma(a)} ) are fixed, \Phi _{a} is already uniquely defined for all polynomials $p(z,\; \backslash overline)\; =\; \backslash sum\_^N\; c\_\; z^k\backslash overline^l\; \backslash ;\; \backslash left(c\_\; \backslash in\; \backslash C\; \backslash right)$, since \Phi _{a} is a *-homomorphism. These form a dense subalgebra of C(\sigma(a)) by the Stone-Weierstrass theorem. Thus \Phi _{a} is

In functional analysis, the continuous functional calculus for a normal operator

T is often of interest, i.e. the case where l{A} is the C*-algebra l{B}(H) of bounded operators on a Hilbert space In the literature, the continuous functional calculus is often only proved for self-adjoint operators in this setting. In this case, the proof does not need the Gelfand

Further properties of the continuous functional calculus

The continuous functional calculus

\Phi _{a} is an isometric isomorphism into the C*-subalgebra C ^{*(a,e)} generated by a and e , that is:\left\| \Phi _{a(f)} \right\| = \left\| f \right\| _{\sigma(a)} for all f \in C(\sigma(a)) ; \Phi _{a} is therefore continuous.\Phi _{a} \left( C(\sigma(a)) \right) = C ^{*(a,} e) \subseteq l{A}

Since

a is a normal element of l{A} , the C*-subalgebra generated by a and e is commutative. In particular, f(a) is normal and all elements of a functional calculus

The holomorphic functional calculus is extended by the continuous functional calculus in an unambiguous Therefore, for polynomials

p(z,\overline{z}) the continuous functional calculus corresponds to the natural functional calculus for polynomials: $\backslash Phi\_a(p(z,\; \backslash overline))\; =\; p(a,\; a^*)\; =\; \backslash sum\_^N\; c\_\; a^k(a^*)^l$ for all

For a sequence of functions

f _{n} \in C(\sigma(a)) that converges uniformly on \sigma(a) to a function f \in C(\sigma(a)) , f _{n(a)} converges to For a power series $f(z)\; =\; \backslash sum\_^\backslash infty\; c\_n\; z^n$, which converges absolutely uniformly on \sigma(a) , therefore $f(a)\; =\; \backslash sum\_^\backslash infty\; c\_na^n$

If

f \in l{C}(\sigma(a)) and g\in l{ C}(\sigma(f(a))) , then (g \circ f)(a) = g(f(a)) holds for their If a,b \in l{A} _{N} are two normal elements with f(a) = f(b) and g is the inverse function of f on both \sigma(a) and \sigma(b) , then a = b , since

The spectral mapping theorem applies:

\sigma(f(a)) = f(\sigma(a)) for all

If

ab = ba holds for b \in l{A} , then f(a)b = bf(a) also holds for all f \in C ( \sigma (a)) , i.e. if b commutates with a , then also with the corresponding elements of the continuous functional calculus

Let

\Psi \colon l{A} → l{B} be an unital *-homomorphism between C*-algebras l{A} and Then \Psi commutates with the continuous functional calculus. The following holds: \Psi(f(a)) = f(\Psi(a)) for all In particular, the continuous functional calculus commutates with the Gelfand

With the spectral mapping theorem, functions with certain properties can be directly related to certain properties of elements of C*-algebras:

f(a) is invertible if and only if f has no zero on Then $f(a)^\; =\; \backslash tfrac\; (a)$ f(a) is self-adjoint if and only if f is real-valued, i.e. f(a) is positive (f(a) \geq 0 ) if and only if f \geq 0 , i.e. f(a) is unitary if all values of f lie in the circle group, i.e. f(a) is a projection if f only takes on the values 0 and 1 , i.e.

These are based on statements about the spectrum of certain elements, which are shown in the Applications section.

In the special case that

l{A} is the C*-algebra of bounded operators l{B}(H) for a Hilbert space H , eigenvectors v \in H for the eigenvalue λ \in \sigma(T) of a normal operator T \in l{B}(H) are also eigenvectors for the eigenvalue f( λ ) \in \sigma(f(T)) of the operator If Tv = λ v , then f(T)v = f( λ )v also holds for all

Applications

The following applications are typical and very simple examples of the numerous applications of the continuous functional calculus:

Spectrum

Let

l{A} be a C*-algebra and a \in l{A} _{N} a normal element. Then the following applies to the spectrum a is self-adjoint if and only if a is unitary if and only if a is a projection if and only if

Proof. The continuous functional calculus

\Phi _{a} for the normal element a \in l{A} is a *-homomorphism with \Phi _{a} (\operatorname{Id}) = a and thus a is self-adjoint/unitary/a projection if \operatorname{Id} \in C( \sigma(a)) is also self-adjoint/unitary/a projection. Exactly then \operatorname{Id} is self-adjoint if z = Id (z) = \overline{ Id }(z) = \overline holds for all z \in \sigma(a) , i.e. if \sigma(a) is real. Exactly then Id is unitary if 1 = Id (z) \overline{\operatorname{Id}}(z) = z \overline{z} = |z| ^{2} holds for all z \in \sigma(a) , therefore Exactly then Id is a projection if and only if (\operatorname{Id}(z)) ^{2} = \operatorname{Id}}(z) = \overline{\operatorname{Id}(z) , that is z ^{2} = z = \overline{z} for all z \in \sigma(a) , i.e. \sigma(a) \subseteq \{ 0 , 1 \}

Roots

Let

a be a positive element of a C*-algebra Then for every n \in N there exists a uniquely determined positive element b \in l{A} _{+} with b ^{n} = a , i.e. a unique n -th

Proof. For each

n \in N , the root function f _{n} \colon \R ^{+} _{0} \to \R ^{+ ,} _{0} x \mapsto \sqrt[n]x is a continuous function on If b \colon = f _{n} (a) is defined using the continuous functional calculus, then b ^{n} = (f ^{n} _{n(a))} = (f ^{n)(a)} _{n} = \operatorname{Id} _{\sigma(a)} (a) = a follows from the properties of the calculus. From the spectral mapping theorem follows \sigma(b) = \sigma(f _{n(a))} = f _{n(\sigma(a))} \subseteq [ 0 , inf ty) , i.e. b is If c \in l{A} _{+} is another positive element with c ^{n} = a = b ^{n} , then c = f _{n} (c ^{n)} = f ^{n)} _{n(b} = b holds, as the root function on the positive real numbers is an inverse function to the function

If

a \in l{A} _{sa} is a self-adjoint element, then at least for every odd n \in \N there is a uniquely determined self-adjoint element b \in l{A} _{sa} with

Similarly, for a positive element

a of a C*-algebra l{A} , each \alpha \geq 0 defines a uniquely determined positive element a ^{\alpha} of C ^{*(a)} , such that a ^{\alpha} a ^{\beta} = a ^{\alpha} holds for all If a is invertible, this can also be extended to negative values of

Absolute value

If

a \in l{A} , then the element a ^{*a} is positive, so that the absolute value can be defined by the continuous functional calculus |a| = \sqrt{a ^{*a}} , since it is continuous on the positive real

Let

a be a self-adjoint element of a C*-algebra l{A} , then there exist positive elements a _{+,a} _{-} \in l{A} _{+} , such that a = a _{+} - a _{-} with a _{+} a _{-} = a _{-} a _{+} = 0 holds. The elements a _{+} and a _{-} are also referred to as the In addition, |a| = a _{+} + a _{-}

Proof. The functions

f _{+(z)} = max (z, 0 ) and f _{-(z)} = -min (z, 0 ) are continuous functions on \sigma(a) \subseteq \R with \operatorname{Id} (z) = z = f _{+(z)} - f _{-(z)} and Put a _{+} = f _{+(a)} and a _{-} = f _{-(a)} . According to the spectral mapping theorem, a _{+} and a _{-} are positive elements for which a = \operatorname{Id}(a) = (f _{+} - f _{-)} (a) = f _{+(a)} - f _{-(a)} = a _{+} - a _{-} and a _{+} a _{-} = f _{+(a)f} _{-(a)} = (f _{+f} _{-)(a)} = 0 = (f _{-f} _{+)(a)} = f _{-(a)f} _{+(a)} = a _{-} a _{+} Furthermore, $f\_+(z)\; +\; f\_-(z)\; =\; |z|\; =\; \backslash sqrt\; =\; \backslash sqrt$, such that

Unitary elements

If

a is a self-adjoint element of a C*-algebra l{A} with unit element e , then u = e ^{i} is unitary, where i denotes the imaginary unit. Conversely, if u \in l{A} _{U} is an unitary element, with the restriction that the spectrum is a proper subset of the unit circle, i.e. \sigma(u) \subsetneq T , there exists a self-adjoint element a \in l{A} _{sa} with

Proof. It is

u = f(a) with f \colon \R \to \C, x \mapsto e ^{ix} , since a is self-adjoint, it follows that \sigma(a) \subset \R , i.e. f is a function on the spectrum of Since f ⋅ \overline{f} = \overline{f} ⋅ f = 1 , using the functional calculus uu ^{*} = u ^{*u} = e follows, i.e. u is unitary. Since for the other statement there is a z _{0} \in T , such that \sigma(u) \subseteq \{ e ^{i} \mid z _{0} \leq z \leq z _{0} + 2 \pi \} the function f( e ^{i} ) = z is a real-valued continuous function on the spectrum \sigma(u) for z _{0} \leq z \leq z _{0} + 2 \pi , such that a = f(u) is a self-adjoint element that satisfies

Spectral decomposition theorem

Let

l{A} be an unital C*-algebra and a \in l{A} _{N} a normal element. Let the spectrum consist of n pairwise disjoint closed subsets \sigma _{k} \subset \C for all 1 \leq k \leq n , i.e. Then there exist projections p _{1,} \ldots, p _{n} \in l{A} that have the following properties for all

• For the spectrum,

\sigma(p _{k)} = \sigma _{k} holds.

• The projections commutate with

a , i.e.

• The projections are orthogonal, i.e.
• The sum of the projections is the unit element, i.e.

In particular, there is a decomposition $a\; =\; \backslash sum\_^n\; a\_k$ for which

\sigma(a _{k)} = \sigma _{k} holds for all

Proof. Since all

\sigma _{k} are closed, the characteristic functions \chi _{\sigma _{k}} are continuous on Now let p _{k} : = \chi _{\sigma _{k}} (a) be defined using the continuous functional. As the \sigma _{k} are pairwise disjoint, \chi _{\sigma _{j}} \chi _{\sigma _{k}} = \delta _{jk} \chi _{\sigma _{k}} and $\backslash sum\_^n\; \backslash chi\_\; =\; \backslash chi\_\; =\; \backslash chi\_\; =\; \backslash textbf$ holds and thus the p _{k} satisfy the claimed properties, as can be seen from the properties of the continuous functional equation. For the last statement, let

References

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External links

• Continuous functional calculus on PlanetMath