Continuous functional calculus

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

If one wants to extend the natural functional calculus for polynomials on the spectrum <math>\sigma(a)</math> of an element <math>a</math> of a Banach algebra <math>\mathcal{A}</math> to a functional calculus for continuous functions <math>C(\sigma(a))</math> 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 Template:Nowrap The continuous functions on <math>\sigma(a) \subset \C</math> are approximated by polynomials in <math>z</math> and <math>\overline{z}</math>, i.e. by polynomials of the form Template:Nowrap Here, <math>\overline{z}</math> denotes the complex conjugation, which is an involution on the Template:Nowrap To be able to insert <math>a</math> in place of <math>z</math> in this kind of polynomial, Banach *-algebras are considered, i.e. Banach algebras that also have an involution *, and <math>a^*</math> is inserted in place of Template:Nowrap In order to obtain a homomorphism <math>{\mathbb C}[z,\overline{z}]\rightarrow\mathcal{A}</math>, a restriction to normal elements, i.e. elements with <math>a^*a = aa^*</math>, is necessary, as the polynomial ring <math>\C[z,\overline{z}]</math> is commutative. If <math>(p_n(z,\overline{z}))_n</math> is a sequence of polynomials that converges uniformly on <math>\sigma(a)</math> to a continuous function <math>f</math>, the convergence of the sequence <math>(p_n(a,a^*))_n</math> in <math>\mathcal{A}</math> to an element <math>f(a)</math> 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 <math>f,g \in C(\sigma(a))</math> and scalars <math>\lambda,\mu \in \C</math>:Template:Sfn

<math>(\lambda f + \mu g)(a) = \lambda f(a) + \mu g(a) \qquad</math>	(linear)
<math>(f \cdot g)(a) = f (a) \cdot g(a)</math>	(multiplicative)
<math>\overline{f}(a) =\colon \; (f^*)(a) = (f(a))^*</math>	(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 Template:Nowrap Then if <math>a \in \mathcal{A}</math> and <math>f \in C(\sigma (a))</math> with <math>f(0) = 0</math>, it follows that <math>0 \in \sigma (a)</math> and Template:Nowrap

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

• Existence: Since the spectrum of <math>a</math> in the C*-subalgebra <math>C^*(a,e)</math> generated by <math>a</math> and <math>e</math> is the same as it is in <math>\mathcal{A}</math>, it suffices to show the statement for Template:Nowrap The actual construction is almost immediate from the Gelfand representation: it suffices to assume <math>\mathcal{A}</math> is the C*-algebra of continuous functions on some compact space <math>X</math> and define Template:Nowrap

• Uniqueness: Since <math>\Phi_a(\boldsymbol{1})</math> and <math>\Phi_a(\operatorname{Id}_{\sigma(a)})</math> are fixed, <math>\Phi_a</math> is already uniquely defined for all polynomials <math display="inline">p(z, \overline{z}) = \sum_{k,l=0}^N c_{k,l} z^k\overline{z}^l \; \left( c_{k,l} \in \C \right)</math>, since <math>\Phi_a</math> is a *-homomorphism. These form a dense subalgebra of <math>C(\sigma(a))</math> by the Stone-Weierstrass theorem. Thus <math>\Phi_a</math> is Template:Nowrap

In functional analysis, the continuous functional calculus for a normal operator <math>T</math> is often of interest, i.e. the case where <math>\mathcal{A}</math> is the C*-algebra <math>\mathcal{B}(H)</math> of bounded operators on a Hilbert space Template:Nowrap 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 Template:Nowrap

Further properties of the continuous functional calculus

The continuous functional calculus <math>\Phi_a</math> is an isometric isomorphism into the C*-subalgebra <math>C^*(a,e)</math> generated by <math>a</math> and <math>e</math>, that is:Template:Sfn

• <math>\left\| \Phi_a(f) \right\| = \left\| f \right\|_{\sigma(a)}</math> for all <math>f \in C(\sigma(a))</math>; <math>\Phi_a</math> is therefore continuous.
• <math>\Phi_a \left( C(\sigma(a)) \right) = C^*(a, e) \subseteq \mathcal{A}</math>

Since <math>a</math> is a normal element of <math>\mathcal{A}</math>, the C*-subalgebra generated by <math>a</math> and <math>e</math> is commutative. In particular, <math>f(a)</math> is normal and all elements of a functional calculus Template:Nowrap

The holomorphic functional calculus is extended by the continuous functional calculus in an unambiguous Template:Nowrap Therefore, for polynomials <math>p(z,\overline{z})</math> the continuous functional calculus corresponds to the natural functional calculus for polynomials: <math display="inline">\Phi_a(p(z, \overline{z})) = p(a, a^*) = \sum_{k,l=0}^N c_{k, l} a^k(a^*)^l</math> for all Template:Nowrap

For a sequence of functions <math>f_n \in C(\sigma(a))</math> that converges uniformly on <math>\sigma(a)</math> to a function <math>f \in C(\sigma(a))</math>, <math>f_n(a)</math> converges to Template:NowrapTemplate:Sfn For a power series <math display="inline">f(z) = \sum_{n=0}^\infty c_n z^n</math>, which converges absolutely uniformly on <math>\sigma(a)</math>, therefore <math display="inline">f(a) = \sum_{n=0}^\infty c_na^n</math> Template:Nowrap

If <math>f \in \mathcal{C}(\sigma(a))</math> and <math>g\in \mathcal{ C}(\sigma(f(a)))</math>, then <math>(g \circ f)(a) = g(f(a))</math> holds for their Template:Nowrap If <math>a,b \in \mathcal{A}_N</math> are two normal elements with <math>f(a) = f(b)</math> and <math>g</math> is the inverse function of <math>f</math> on both <math>\sigma(a)</math> and <math>\sigma(b)</math>, then <math>a = b</math>, since Template:Nowrap

The spectral mapping theorem applies: <math>\sigma(f(a)) = f(\sigma(a))</math> for all Template:Nowrap

If <math>ab = ba</math> holds for <math>b \in \mathcal{A}</math>, then <math>f(a)b = bf(a)</math> also holds for all <math>f \in C ( \sigma (a))</math>, i.e. if <math>b</math> commutates with <math>a</math>, then also with the corresponding elements of the continuous functional calculus Template:Nowrap

Let <math>\Psi \colon \mathcal{A} \rightarrow \mathcal{B}</math> be an unital *-homomorphism between C*-algebras <math>\mathcal{A}</math> and Template:Nowrap Then <math>\Psi</math> commutates with the continuous functional calculus. The following holds: <math>\Psi(f(a)) = f(\Psi(a))</math> for all Template:Nowrap In particular, the continuous functional calculus commutates with the Gelfand Template:Nowrap

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

• <math>f(a)</math> is invertible if and only if <math>f</math> has no zero on Template:Nowrap Then <math display="inline">f(a)^{-1} = \tfrac{1}{f} (a)</math> Template:Nowrap

• <math>f(a)</math> is self-adjoint if and only if <math>f</math> is real-valued, i.e. Template:Nowrap
• <math>f(a)</math> is positive (<math>f(a) \geq 0</math>) if and only if <math>f \geq 0</math>, i.e. Template:Nowrap
• <math>f(a)</math> is unitary if all values of <math>f</math> lie in the circle group, i.e. Template:Nowrap
• <math>f(a)</math> is a projection if <math>f</math> only takes on the values <math>0</math> and <math>1</math>, i.e. Template:Nowrap

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

In the special case that <math>\mathcal{A}</math> is the C*-algebra of bounded operators <math>\mathcal{B}(H)</math> for a Hilbert space <math>H</math>, eigenvectors <math>v \in H</math> for the eigenvalue <math>\lambda \in \sigma(T)</math> of a normal operator <math>T \in \mathcal{B}(H)</math> are also eigenvectors for the eigenvalue <math>f(\lambda) \in \sigma(f(T))</math> of the operator Template:Nowrap If <math>Tv = \lambda v</math>, then <math>f(T)v = f(\lambda)v</math> also holds for all Template:Nowrap

Applications

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

Spectrum

Let <math>\mathcal{A}</math> be a C*-algebra and <math>a \in \mathcal{A}_N</math> a normal element. Then the following applies to the spectrum Template:Nowrap

• <math>a</math> is self-adjoint if and only if Template:Nowrap
• <math>a</math> is unitary if and only if Template:Nowrap
• <math>a</math> is a projection if and only if Template:Nowrap

Proof.Template:Sfn The continuous functional calculus <math>\Phi_a</math> for the normal element <math>a \in \mathcal{A}</math> is a *-homomorphism with <math>\Phi_a (\operatorname{Id}) = a</math> and thus <math>a</math> is self-adjoint/unitary/a projection if <math>\operatorname{Id} \in C( \sigma(a))</math> is also self-adjoint/unitary/a projection. Exactly then <math>\operatorname{Id}</math> is self-adjoint if <math>z = \text{Id}(z) = \overline{\text{Id}}(z) = \overline{z}</math> holds for all <math>z \in \sigma(a)</math>, i.e. if <math>\sigma(a)</math> is real. Exactly then <math>\text{Id}</math> is unitary if <math>1 = \text{Id}(z) \overline{\operatorname{Id}}(z) = z \overline{z} = |z|^2</math> holds for all <math>z \in \sigma(a)</math>, therefore Template:Nowrap Exactly then <math>\text{Id}</math> is a projection if and only if <math>(\operatorname{Id}(z))^2 = \operatorname{Id}}(z) = \overline{\operatorname{Id}(z)</math>, that is <math>z^2 = z = \overline{z}</math> for all <math>z \in \sigma(a)</math>, i.e. <math>\sigma(a) \subseteq \{ 0,1 \}</math>

Roots

Let <math>a</math> be a positive element of a C*-algebra Template:Nowrap Then for every <math>n \in \mathbb{N}</math> there exists a uniquely determined positive element <math>b \in \mathcal{A}_+</math> with <math>b^n =a</math>, i.e. a unique <math>n</math>-th Template:Nowrap

Proof. For each <math>n \in \mathbb{N}</math>, the root function <math>f_n \colon \R_0^+ \to \R_0^+, x \mapsto \sqrt[n]x</math> is a continuous function on Template:Nowrap If <math>b \; \colon = f_n (a)</math> is defined using the continuous functional calculus, then <math>b^n = (f_n(a))^n = (f_n^n)(a) = \operatorname{Id}_{\sigma(a)}(a)=a</math> follows from the properties of the calculus. From the spectral mapping theorem follows <math>\sigma(b) = \sigma(f_n(a)) = f_n(\sigma(a)) \subseteq [0,\infty)</math>, i.e. <math>b</math> is Template:Nowrap If <math>c \in \mathcal{A}_+</math> is another positive element with <math>c^n = a = b^n</math>, then <math>c = f_n (c^n) = f_n(b^n) = b</math> holds, as the root function on the positive real numbers is an inverse function to the function Template:Nowrap

If <math>a \in \mathcal{A}_{sa}</math> is a self-adjoint element, then at least for every odd <math>n \in \N</math> there is a uniquely determined self-adjoint element <math>b \in \mathcal{A}_{sa}</math> with Template:Nowrap

Similarly, for a positive element <math>a</math> of a C*-algebra <math>\mathcal{A}</math>, each <math>\alpha \geq 0</math> defines a uniquely determined positive element <math>a^\alpha</math> of <math>C^*(a)</math>, such that <math>a^\alpha a^\beta = a^{\alpha + \beta}</math> holds for all Template:Nowrap If <math>a</math> is invertible, this can also be extended to negative values of Template:Nowrap

Absolute value

If <math>a \in \mathcal{A}</math>, then the element <math>a^*a</math> is positive, so that the absolute value can be defined by the continuous functional calculus <math>|a| = \sqrt{a^*a}</math>, since it is continuous on the positive real Template:Nowrap

Let <math>a</math> be a self-adjoint element of a C*-algebra <math>\mathcal{A}</math>, then there exist positive elements <math>a_+,a_- \in \mathcal{A}_+</math>, such that <math>a = a_+ - a_-</math> with <math>a_+ a_- = a_- a_+ = 0</math> holds. The elements <math>a_+</math> and <math>a_-</math> are also referred to as the Template:Nowrap In addition, <math>|a| = a_+ + a_-</math> Template:Nowrap

Proof. The functions <math>f_+(z) = \max(z,0)</math> and <math>f_-(z) = -\min(z, 0)</math> are continuous functions on <math>\sigma(a) \subseteq \R</math> with <math>\operatorname{Id} (z) = z = f_+(z) -f_-(z)</math> and Template:Nowrap Put <math>a_+ = f_+(a)</math> and <math>a_- = f_-(a)</math>. According to the spectral mapping theorem, <math>a_+</math> and <math>a_-</math> are positive elements for which <math>a = \operatorname{Id}(a) = (f_+ - f_-) (a) = f_+(a) - f_-(a) = a_+ - a_-</math> and <math>a_+ a_- = f_+(a)f_-(a) = (f_+f_-)(a) = 0 = (f_-f_+)(a) = f_-(a)f_+(a) = a_- a_+</math> Template:Nowrap Furthermore, <math display="inline">f_+(z) + f_-(z) = |z| = \sqrt{z^* z} = \sqrt{z^2}</math>, such that Template:Nowrap

Unitary elements

If <math>a</math> is a self-adjoint element of a C*-algebra <math>\mathcal{A}</math> with unit element <math>e</math>, then <math>u = \mathrm{e}^{\mathrm{i} a}</math> is unitary, where <math>\mathrm{i}</math> denotes the imaginary unit. Conversely, if <math>u \in \mathcal{A}_U</math> is an unitary element, with the restriction that the spectrum is a proper subset of the unit circle, i.e. <math>\sigma(u) \subsetneq \mathbb{T}</math>, there exists a self-adjoint element <math>a \in \mathcal{A}_{sa}</math> with Template:Nowrap

Proof.Template:Sfn It is <math>u = f(a)</math> with <math>f \colon \R \to \C,\ x \mapsto \mathrm{e}^{\mathrm{i}x}</math>, since <math>a</math> is self-adjoint, it follows that <math>\sigma(a) \subset \R</math>, i.e. <math>f</math> is a function on the spectrum of Template:Nowrap Since <math>f\cdot \overline{f} = \overline{f}\cdot f = 1</math>, using the functional calculus <math>uu^* = u^*u = e</math> follows, i.e. <math>u</math> is unitary. Since for the other statement there is a <math>z_0 \in \mathbb{T}</math>, such that <math>\sigma(u) \subseteq \{ \mathrm{e}^{\mathrm{i} z} \mid z_0 \leq z \leq z_0 + 2 \pi \}</math> the function <math>f(\mathrm{e}^{\mathrm{i} z}) = z</math> is a real-valued continuous function on the spectrum <math>\sigma(u)</math> for <math>z_0 \leq z \leq z_0 + 2 \pi</math>, such that <math>a = f(u)</math> is a self-adjoint element that satisfies Template:Nowrap

Spectral decomposition theorem

Let <math>\mathcal{A}</math> be an unital C*-algebra and <math>a \in \mathcal{A}_N</math> a normal element. Let the spectrum consist of <math>n</math> pairwise disjoint closed subsets <math>\sigma_k \subset \C</math> for all <math>1 \leq k \leq n</math>, i.e. Template:Nowrap Then there exist projections <math>p_1, \ldots, p_n \in \mathcal{A}</math> that have the following properties for all Template:Nowrap

• For the spectrum, <math>\sigma(p_k) = \sigma_k</math> holds.
• The projections commutate with <math>a</math>, i.e. Template:Nowrap
• The projections are orthogonal, i.e. Template:Nowrap
• The sum of the projections is the unit element, i.e. Template:Nowrap

In particular, there is a decomposition <math display="inline">a = \sum_{k=1}^n a_k</math> for which <math>\sigma(a_k) = \sigma_k</math> holds for all Template:Nowrap

Proof.Template:Sfn Since all <math>\sigma_k</math> are closed, the characteristic functions <math>\chi_{\sigma_k}</math> are continuous on Template:Nowrap Now let <math>p_k := \chi_{\sigma_k} (a)</math> be defined using the continuous functional. As the <math>\sigma_k</math> are pairwise disjoint, <math>\chi_{\sigma_j} \chi_{\sigma_k} = \delta_{jk} \chi_{\sigma_k}</math> and <math display="inline">\sum_{k=1}^n \chi_{\sigma_k} = \chi_{\cup_{k=1}^n \sigma_k} = \chi_{\sigma(a)} = \textbf{1}</math> holds and thus the <math>p_k</math> satisfy the claimed properties, as can be seen from the properties of the continuous functional equation. For the last statement, let Template:Nowrap

References

• Template:Cite book
• Template:Cite book
• Template:Cite book
• Template:Cite book English translation of Template:Cite book
• Template:Cite book
• Template:Cite book
• Template:Cite book
• Template:Cite book
• Template:Cite book
• Template:Cite book

External links

• Continuous functional calculus on PlanetMath