The Dual of C(X): Riesz Representation

Complex Measures & Total Variation Regular Borel Measures and M(X) From Functionals to Measures The Riesz Representation Theorem

Complex Measures & Total Variation

Two of the function spaces we have dualized return their own kind: the dual of a Hilbert space is again a space of vectors through the Riesz Representation Theorem, and the dual of \(L^p\) is the conjugate space \(L^q\). The continuous functions on a compact space behave differently. A continuous linear functional on \(C(X)\) cannot in general be written as integration against an \(L^q\) density, because \(C(X)\) carries the supremum norm and its dual must account for evaluation-like behavior concentrated on small sets. The objects that do the work are measures: the dual of \(C(X)\) turns out to be a space of measures on \(X\), with the functional acting by integration \(f \mapsto \int f \, d\mu\). The goal of this page is to make that identification precise and to prove it.

Establishing this requires measures that may take complex values, since the functionals on \(C(X)\) are complex-linear. We therefore begin by extending the notion of a signed measure to the complex setting and by constructing the total variation, the device that measures the size of such an object and ultimately supplies the dual norm. We work over a compact (or, where noted, locally compact) Hausdorff space \(X\), and we write \(\Omega\) for a \(\sigma\)-algebra of subsets of \(X\).

Recall the real-valued notion: a signed measure on a measurable space \((X, \Omega)\) is a countably additive set function \(\nu : \Omega \to [-\infty, \infty]\) with \(\nu(\varnothing) = 0\), assuming at most one of the values \(\pm\infty\). The complex case removes the infinite values entirely, since the sum of a convergent complex series must be finite.

Definition: Complex Measure

Let \((X, \Omega)\) be a measurable space. A complex measure on \((X, \Omega)\) is a function \(\mu : \Omega \to \mathbb{C}\) that is countably additive: for every sequence \((A_n)_{n \geq 1}\) of pairwise disjoint sets in \(\Omega\), \[ \mu\!\left(\bigsqcup_{n=1}^\infty A_n\right) \;=\; \sum_{n=1}^\infty \mu(A_n), \] the series converging in \(\mathbb{C}\). Taking all \(A_n = \varnothing\) for \(n \geq 2\) forces \(\mu(\varnothing) = 0\). A complex measure takes only finite values by definition.

Writing \(\mu = \operatorname{Re}\mu + i \operatorname{Im}\mu\), the real and imaginary parts \((\operatorname{Re}\mu)(\Delta) = \operatorname{Re}\bigl(\mu(\Delta)\bigr)\) and \((\operatorname{Im}\mu)(\Delta) = \operatorname{Im}\bigl(\mu(\Delta)\bigr)\) are each real-valued and countably additive, hence finite signed measures. Applying the Jordan decomposition to each gives four positive finite measures \(\mu_1, \mu_2, \mu_3, \mu_4\) with \[ \mu \;=\; (\mu_1 - \mu_2) + i(\mu_3 - \mu_4), \] where \(\mu_1 \perp \mu_2\) and \(\mu_3 \perp \mu_4\) are mutually singular. A real-valued signed measure that happens to be finite is the special case \(\operatorname{Im}\mu = 0\); the development below therefore subsumes the real theory, with the four-measure decomposition collapsing to the two-measure Jordan form.

The Total Variation

For a finite signed measure the total variation is defined through the Jordan decomposition as \(|\nu| = \nu^+ + \nu^-\). A complex measure has no such order structure, so we take instead the supremum-over-partitions description, which agrees with \(\nu^+ + \nu^-\) in the real case and extends verbatim to the complex one.

Definition: Total Variation of a Complex Measure

Let \(\mu\) be a complex measure on \((X, \Omega)\). The total variation of \(\mu\) is the set function \(|\mu| : \Omega \to [0, \infty]\) defined by \[ |\mu|(\Delta) \;=\; \sup\left\{\, \sum_{j=1}^{m} |\mu(E_j)| \;:\; \{E_j\}_{j=1}^{m} \text{ is a measurable partition of } \Delta \,\right\}, \] the supremum running over all finite partitions of \(\Delta\) into pairwise disjoint measurable sets.

For a finite signed measure \(\nu\), choosing the partition \(\{P \cap \Delta,\, N \cap \Delta\}\) given by a Hahn decomposition \(X = P \sqcup N\) yields \(\sum_j |\nu(E_j)| = \nu^+(\Delta) + \nu^-(\Delta) = |\nu|(\Delta)\). No partition can exceed this: for any measurable \(E_j\), the values \(\nu^+(E_j)\) and \(\nu^-(E_j)\) are nonnegative, so \[ |\nu(E_j)| \;=\; |\nu^+(E_j) - \nu^-(E_j)| \;\leq\; \nu^+(E_j) + \nu^-(E_j), \] and summing over any partition \(\{E_j\}\) of \(\Delta\) gives \(\sum_j |\nu(E_j)| \leq \nu^+(\Delta) + \nu^-(\Delta)\) by additivity of \(\nu^+\) and \(\nu^-\). The supremum definition thus recovers \(\nu^+ + \nu^-\), confirming the two notions coincide where both apply.

The central structural fact is that this supremum is itself a measure, and a finite one. The finiteness is the substantive part: it is what makes the dual norm well defined.

Theorem: The Total Variation is a Finite Positive Measure

Let \(\mu\) be a complex measure on \((X, \Omega)\). Then \(|\mu|\) is a positive measure on \((X, \Omega)\), and it is finite: \(|\mu|(X) < \infty\).

Proof

Countable additivity.
Let \(\Delta = \bigsqcup_{n=1}^\infty \Delta_n\) be a disjoint union of measurable sets. We show \(|\mu|(\Delta) = \sum_n |\mu|(\Delta_n)\).

For the inequality \(|\mu|(\Delta) \leq \sum_n |\mu|(\Delta_n)\), let \(\{E_j\}_{j=1}^m\) be any finite measurable partition of \(\Delta\). Each \(E_j = \bigsqcup_n (E_j \cap \Delta_n)\), so by countable additivity of \(\mu\) and the triangle inequality, \[ \sum_{j=1}^m |\mu(E_j)| \;=\; \sum_{j=1}^m \left| \sum_{n=1}^\infty \mu(E_j \cap \Delta_n) \right| \;\leq\; \sum_{j=1}^m \sum_{n=1}^\infty |\mu(E_j \cap \Delta_n)| \;=\; \sum_{n=1}^\infty \sum_{j=1}^m |\mu(E_j \cap \Delta_n)|. \] For each fixed \(n\), the sets \(\{E_j \cap \Delta_n\}_{j=1}^m\) form a measurable partition of \(\Delta_n\), so \(\sum_{j=1}^m |\mu(E_j \cap \Delta_n)| \leq |\mu|(\Delta_n)\). Hence \(\sum_{j=1}^m |\mu(E_j)| \leq \sum_{n=1}^\infty |\mu|(\Delta_n)\). Taking the supremum over all partitions \(\{E_j\}\) of \(\Delta\) gives \(|\mu|(\Delta) \leq \sum_{n=1}^\infty |\mu|(\Delta_n)\).

For the reverse inequality \(|\mu|(\Delta) \geq \sum_n |\mu|(\Delta_n)\), fix \(N \geq 1\) and \(\varepsilon > 0\). For each \(n \leq N\) choose a measurable partition \(\{E^{(n)}_j\}_j\) of \(\Delta_n\) with \(\sum_j |\mu(E^{(n)}_j)| > |\mu|(\Delta_n) - \varepsilon / 2^n\). The collection \(\{E^{(n)}_j : 1 \leq n \leq N,\, j\} \cup \{\Delta \setminus \bigsqcup_{n \leq N} \Delta_n\}\) is a finite measurable partition of \(\Delta\), so \[ |\mu|(\Delta) \;\geq\; \sum_{n=1}^N \sum_j |\mu(E^{(n)}_j)| \;>\; \sum_{n=1}^N \left( |\mu|(\Delta_n) - \frac{\varepsilon}{2^n} \right) \;>\; \sum_{n=1}^N |\mu|(\Delta_n) - \varepsilon. \] Letting \(\varepsilon \to 0\) gives \(|\mu|(\Delta) \geq \sum_{n=1}^N |\mu|(\Delta_n)\), and then \(N \to \infty\) gives \(|\mu|(\Delta) \geq \sum_{n=1}^\infty |\mu|(\Delta_n)\). Combined with the first inequality, \(|\mu|\) is countably additive. Since \(|\mu|(\varnothing) = 0\) and \(|\mu| \geq 0\), it is a positive measure.

Finiteness.
Decompose \(\mu = (\mu_1 - \mu_2) + i(\mu_3 - \mu_4)\) into four positive finite measures as above. For any measurable \(E\), \[ |\mu(E)| \;=\; \bigl| (\mu_1 - \mu_2)(E) + i(\mu_3 - \mu_4)(E) \bigr| \;\leq\; \mu_1(E) + \mu_2(E) + \mu_3(E) + \mu_4(E). \] Hence for any finite partition \(\{E_j\}\) of \(X\), \[ \sum_j |\mu(E_j)| \;\leq\; \sum_j \sum_{k=1}^4 \mu_k(E_j) \;=\; \sum_{k=1}^4 \mu_k(X), \] the last equality by additivity of each \(\mu_k\). Taking the supremum over partitions, \(|\mu|(X) \leq \mu_1(X) + \mu_2(X) + \mu_3(X) + \mu_4(X) < \infty\), since each \(\mu_k\) is finite.

The finiteness argument also shows \(|\mu(E)| \leq |\mu|(E)\) for every measurable \(E\), taking the trivial partition \(\{E\}\) in the definition. The total variation therefore dominates \(\mu\) setwise while being a genuine positive measure, and it assigns to all of \(X\) a finite number — the quantity that will serve as the norm of \(\mu\).

Regular Borel Measures and M(X)

A complex measure as defined above lives on an abstract measurable space. To represent functionals on \(C(X)\) we need measures that interact correctly with the topology of \(X\): the mass of a set must be approximable by the mass of compact sets from inside and open sets from outside. These regularity conditions tie the measure to the topology and are what make the representation unique. We now place the measures on the natural \(\sigma\)-algebra and impose regularity.

Throughout, \(X\) is a locally compact Hausdorff space. The Borel \(\sigma\)-algebra \(\Omega\) is the smallest \(\sigma\)-algebra of subsets of \(X\) containing all open sets; its members are the Borel sets. A compact subset and an open subset of \(X\) are Borel, so the approximation conditions below are well posed.

Definition: Regular Borel Measure

Let \(X\) be a locally compact Hausdorff space with Borel \(\sigma\)-algebra \(\Omega\). A positive measure \(\mu\) on \((X, \Omega)\) is a regular Borel measure if

(a) \(\mu(K) < \infty\) for every compact set \(K \subseteq X\);
(b) \(\mu(E) = \sup\{\, \mu(K) : K \subseteq E,\ K \text{ compact} \,\}\) for every \(E \in \Omega\) (inner regularity);
(c) \(\mu(E) = \inf\{\, \mu(U) : U \supseteq E,\ U \text{ open} \,\}\) for every \(E \in \Omega\) (outer regularity).

A complex measure \(\mu\) on \((X, \Omega)\) is a regular Borel measure if its total variation \(|\mu|\) is a regular Borel measure in the sense above.

When \(X\) is compact, condition (a) is automatic, since \(\mu(X) < \infty\) for any finite measure and every compact set has no greater measure. Conditions (b) and (c) remain the substance: they say a Borel set is squeezed between the compact sets it contains and the open sets that contain it. This is the case relevant to \(C(X)\) on a compact \(X\); the locally compact formulation is stated as primary because the representation theorem and its corollary on \(C_0(X)\) hold at that generality, with the compact case as the specialization \(C_0(X) = C(X)\).

The Space M(X)

The regular Borel measures of finite total variation form a vector space, on which the total variation of the whole space supplies a norm.

Definition: The Space \(M(X)\)

Let \(X\) be a locally compact Hausdorff space. Denote by \(M(X)\) the set of all complex-valued regular Borel measures on \(X\). It is a vector space over \(\mathbb{C}\) under the pointwise operations \((\mu + \nu)(E) = \mu(E) + \nu(E)\) and \((\lambda\mu)(E) = \lambda\,\mu(E)\). For \(\mu \in M(X)\), set \[ \|\mu\| \;=\; |\mu|(X), \] the total variation of \(\mu\) over all of \(X\), which is finite by the preceding section.

That the pointwise operations preserve regularity, and that \(\|\cdot\|\) is a norm, must be checked. We record both as a single proposition.

Proposition: \(M(X)\) is a Normed Space

\(M(X)\) is a complex vector space, and \(\|\mu\| = |\mu|(X)\) defines a norm on it.

Proof

Vector-space structure.
If \(\mu, \nu \in M(X)\) and \(\lambda \in \mathbb{C}\), then \(\mu + \nu\) and \(\lambda\mu\) are complex measures, being pointwise combinations of countably additive set functions. We must check they remain regular, i.e. that \(|\mu + \nu|\) and \(|\lambda\mu|\) are regular Borel measures. From the partition definition, for any \(E\) and any partition \(\{E_j\}\), \[ \sum_j |(\mu + \nu)(E_j)| \;\leq\; \sum_j |\mu(E_j)| + \sum_j |\nu(E_j)| \;\leq\; |\mu|(E) + |\nu|(E), \] so taking the supremum gives \(|\mu + \nu|(E) \leq |\mu|(E) + |\nu|(E)\); that is, \(|\mu + \nu| \leq |\mu| + |\nu|\) setwise. Likewise \(|\lambda\mu| = |\lambda|\,|\mu|\), since each term \(|\lambda\mu(E_j)| = |\lambda|\,|\mu(E_j)|\) scales by \(|\lambda|\).

It remains to deduce that \(|\mu + \nu|\) is regular; the same argument applies to \(|\lambda\mu| = |\lambda|\,|\mu|\), which is regular because a nonnegative scalar multiple of a regular measure is regular. Write \(\rho = |\mu + \nu|\) and \(\sigma = |\mu| + |\nu|\), so that \(\rho \leq \sigma\) setwise. Both are finite positive measures, and \(\sigma\) is regular, being a sum of two regular measures (approximate each summand separately and add). The key elementary fact is this: because \(\rho\) and \(\sigma\) are finite and \(\rho \leq \sigma\), for any two Borel sets \(A \subseteq B\) we have \[ \rho(B) - \rho(A) \;=\; \rho(B \setminus A) \;\leq\; \sigma(B \setminus A), \] so whenever \(\sigma\) approximates a set well, \(\rho\) does too.

Inner regularity. Fix \(E \in \Omega\) and \(\varepsilon > 0\). By inner regularity of \(\sigma\) there is a compact \(K \subseteq E\) with \(\sigma(E \setminus K) < \varepsilon\). Applying the fact above with \(A = K\), \(B = E\), \[ \rho(E) - \rho(K) \;\leq\; \sigma(E \setminus K) \;<\; \varepsilon, \] so \(\rho(K)\) comes within \(\varepsilon\) of \(\rho(E)\). Since \(\varepsilon\) was arbitrary, \(\rho(E) = \sup\{\rho(K) : K \subseteq E,\ K \text{ compact}\}\).

Outer regularity. Similarly, by outer regularity of \(\sigma\) there is an open \(U \supseteq E\) with \(\sigma(U \setminus E) < \varepsilon\), and the fact above with \(A = E\), \(B = U\) gives \(\rho(U) - \rho(E) \leq \sigma(U \setminus E) < \varepsilon\). Hence \(\rho(E) = \inf\{\rho(U) : U \supseteq E,\ U \text{ open}\}\). Thus \(\rho = |\mu + \nu|\) is regular, and \(\mu + \nu, \lambda\mu \in M(X)\).

Positivity and definiteness.
Clearly \(\|\mu\| = |\mu|(X) \geq 0\). If \(\|\mu\| = 0\), then \(|\mu|(X) = 0\), so \(|\mu|(E) = 0\) for every \(E \subseteq X\) by monotonicity; since \(|\mu(E)| \leq |\mu|(E) = 0\), we get \(\mu(E) = 0\) for all \(E\), i.e. \(\mu = 0\). Conversely \(\|0\| = 0\).

Homogeneity.
\(\|\lambda\mu\| = |\lambda\mu|(X) = |\lambda|\,|\mu|(X) = |\lambda|\,\|\mu\|\), using \(|\lambda\mu| = |\lambda|\,|\mu|\) from above.

Triangle inequality.
\(\|\mu + \nu\| = |\mu + \nu|(X) \leq |\mu|(X) + |\nu|(X) = \|\mu\| + \|\nu\|\), using \(|\mu + \nu| \leq |\mu| + |\nu|\) from above. Thus \(\|\cdot\|\) is a norm.

Support and Point Masses

Two further notions attached to a measure will be needed when the representation is applied: the set on which a measure genuinely lives, and the simplest measures of all, concentrated at a single point.

Definition: Support of a Measure

Let \(\mu\) be a complex measure on a locally compact Hausdorff space \(X\) with Borel \(\sigma\)-algebra \(\Omega\). The support of \(\mu\) is the set \[ \operatorname{supp}\mu \;=\; X \setminus \bigcup\{\, V : V \text{ is open and } |\mu|(V) = 0 \,\}. \] Equivalently, \(\operatorname{supp}\mu\) is the smallest closed set whose complement is \(|\mu|\)-null: it is the set of points every open neighborhood of which carries positive total variation.

The complement of \(\operatorname{supp}\mu\) is a union of \(|\mu|\)-null open sets, hence open, so \(\operatorname{supp}\mu\) is closed. Moreover this null complement is itself \(|\mu|\)-null, and crucially no countability of \(X\) is needed: writing \(W = X \setminus \operatorname{supp}\mu\), every compact \(C \subseteq W\) is covered by finitely many of the null open sets whose union is \(W\), so \(|\mu|(C) = 0\); inner regularity of \(|\mu|\) then gives \(|\mu|(W) = \sup\{|\mu|(C) : C \subseteq W \text{ compact}\} = 0\). Consequently \(\int_X f \, d\mu = \int_{\operatorname{supp}\mu} f \, d\mu\) for every integrable \(f\), since the integrand contributes nothing off the support. This is exactly the step that lets one replace \(X\) by the support of a measure without losing any of its mass.

Definition: Dirac Measure

For a point \(x \in X\), the Dirac measure (or point mass) \(\delta_x\) is the positive measure defined by \[ \delta_x(E) \;=\; \begin{cases} 1 & x \in E, \\ 0 & x \notin E, \end{cases} \] for \(E \in \Omega\). It is a regular Borel measure with \(\|\delta_x\| = 1\) and \(\operatorname{supp}\delta_x = \{x\}\), and integration against it is evaluation: \(\int_X f \, d\delta_x = f(x)\) for every \(f \in C(X)\). A scalar multiple \(\alpha\delta_x\) with \(\alpha \in \mathbb{C}\) is the complex measure \(E \mapsto \alpha\,\delta_x(E)\), with \(\|\alpha\delta_x\| = |\alpha|\).

Countable additivity of \(\delta_x\) holds because at most one set in a disjoint family contains \(x\); regularity holds because \(\{x\}\) is compact and the value on any Borel set is determined by whether it contains \(x\). These point masses are the extreme points of the unit ball of \(M(X)\), a fact that surfaces once the representation identifies \(M(X)\) with a dual space.

From Functionals to Measures

We now connect the two sides. One direction is easy and explicit: every measure produces a functional by integration. The other direction — that every functional arises this way — is the substance of the representation theorem and occupies the rest of this section. Throughout, \(C_0(X)\) is the space of continuous functions \(f : X \to \mathbb{C}\) that vanish at infinity, meaning that for each \(\varepsilon > 0\) the set \(\{|f| \geq \varepsilon\}\) is compact, equipped with the supremum norm \(\|f\|_\infty = \sup_x |f(x)|\). When \(X\) is compact this is simply \(C(X)\), since every continuous function then has compact support automatically.

Each Measure Defines a Functional

Lemma: Integration Against a Measure is a Functional

Let \(\mu \in M(X)\) and define \(F_\mu : C_0(X) \to \mathbb{C}\) by \(F_\mu(f) = \int f \, d\mu\). Then \(F_\mu\) is a bounded linear functional, \(F_\mu \in C_0(X)^*\), and \[ \|F_\mu\| \;=\; \|\mu\| \;=\; |\mu|(X). \]

Proof Sketch

Boundedness and the upper estimate (full).
Linearity of \(F_\mu\) is the linearity of the integral. For \(f \in C_0(X)\), the bound \(|f(x)| \leq \|f\|_\infty\) and the inequality \(\left| \int f \, d\mu \right| \leq \int |f| \, d|\mu|\) — which holds because, decomposing into real and imaginary signed parts and then into positive and negative pieces, the integral against \(\mu\) is dominated termwise by the integral of \(|f|\) against \(|\mu|\) — give \[ |F_\mu(f)| \;=\; \left| \int f \, d\mu \right| \;\leq\; \int |f| \, d|\mu| \;\leq\; \|f\|_\infty \, |\mu|(X) \;=\; \|f\|_\infty \, \|\mu\|. \] Hence \(F_\mu\) is bounded with \(\|F_\mu\| \leq \|\mu\|\).

The lower estimate (sketch — it rests on the approximation principle stated after the proof).
For the reverse inequality \(\|F_\mu\| \geq \|\mu\|\) we must produce functions \(f\) with \(\|f\|_\infty \leq 1\) and \(|F_\mu(f)|\) close to \(|\mu|(X)\). The polar decomposition of \(\mu\) writes \(\mu = h \, |\mu|\) for a Borel function \(h\) with \(|h| = 1\) almost everywhere with respect to \(|\mu|\); this is the measure-theoretic statement that \(\mu\) and \(|\mu|\) differ only by a unimodular phase. The natural candidate is \(f = \bar{h}\), for which \[ \int \bar{h} \, d\mu \;=\; \int \bar{h} \, h \, d|\mu| \;=\; \int |h|^2 \, d|\mu| \;=\; |\mu|(X), \] but \(\bar{h}\) is only Borel, not continuous, and need not lie in \(C_0(X)\). The remedy is to approximate \(\bar{h}\) by a continuous function. There is a classical approximation principle: a Borel function that is bounded by \(1\) can, off a set of arbitrarily small \(|\mu|\)-measure, be matched by a continuous function of supremum norm at most \(1\). Granting such an approximant \(\phi\) with \(\|\phi\|_\infty \leq 1\) and \(\int |\phi - \bar{h}| \, d|\mu| < \varepsilon\), we get \[ |F_\mu(\phi)| \;=\; \left| \int \phi \, d\mu \right| \;\geq\; \left| \int \bar{h} \, d\mu \right| - \left| \int (\phi - \bar{h}) \, d\mu \right| \;\geq\; |\mu|(X) - \int |\phi - \bar{h}| \, d|\mu| \;>\; |\mu|(X) - \varepsilon. \] Since \(\|\phi\|_\infty \leq 1\), this forces \(\|F_\mu\| \geq |\mu|(X) - \varepsilon\), and letting \(\varepsilon \to 0\) gives \(\|F_\mu\| \geq \|\mu\| = |\mu|(X)\). With the upper estimate, \(\|F_\mu\| = \|\mu\|\).

The approximation principle used here expresses the regularity of \(|\mu|\) at the level of functions: just as a Borel set is approximable by compact and open sets, a bounded Borel function is approximable, in the mean, by a continuous one of the same supremum bound. We use it as a stated principle; its proof builds the continuous approximant on the compact sets supplied by inner regularity.

The map \(\mu \mapsto F_\mu\) is therefore a norm-preserving linear injection of \(M(X)\) into \(C_0(X)^*\): linear because the integral is linear in the measure, injective because \(\|F_\mu\| = \|\mu\|\) forces \(F_\mu = 0 \Rightarrow \mu = 0\). Surjectivity — recovering a measure from an arbitrary functional — we approach in two steps: first reduce to a positive functional, then realize a positive functional by a positive measure.

Reduction to a Positive Functional

Call a linear functional \(I : C_0(X) \to \mathbb{C}\) positive if \(I(f) \geq 0\) whenever \(f \geq 0\). Positivity is the order-theoretic analogue of being represented by a positive measure, and it is the form in which a measure is easiest to extract. The first step shows every bounded functional dominates a positive one of the same norm.

Lemma: A Bounded Functional Yields a Positive Functional

Let \(F : C_0(X) \to \mathbb{C}\) be a bounded linear functional. For \(f \in C_0(X)\) with \(f \geq 0\), define \[ I(f) \;=\; \sup\{\, |F(g)| : g \in C_0(X),\ |g| \leq f \,\}. \] Then \(I\) extends to a positive linear functional on \(C_0(X)\) with \(\|I\| = \|F\|\) and \(|F(g)| \leq I(|g|)\) for all \(g\).

Proof Sketch

For \(f \geq 0\), the defining supremum is finite because \(|F(g)| \leq \|F\| \, \|g\|_\infty \leq \|F\| \, \|f\|_\infty\) whenever \(|g| \leq f\), so \(0 \leq I(f) \leq \|F\| \, \|f\|_\infty\). Taking \(g = f\) gives \(I(f) \geq |F(f)|\), and the case \(g\) ranging over multiples of \(f\) gives \(I(f) \geq \|F\|\,\|f\|_\infty\) in the limit, so in fact \(\|I\| = \|F\|\). One checks additivity on nonnegative functions: \(I(f_1 + f_2) = I(f_1) + I(f_2)\) for \(f_1, f_2 \geq 0\), the inequality \(\geq\) by combining near-optimal \(g_1, g_2\) into \(g_1 + g_2\) after adjusting phases so that \(|F(g_1)| + |F(g_2)| = |F(g_1 + g_2)|\), and \(\leq\) by splitting any \(g\) with \(|g| \leq f_1 + f_2\) as \(g = g_1 + g_2\) with \(|g_i| \leq f_i\) (set \(g_i = g f_i / (f_1 + f_2)\) where the denominator is positive, \(0\) elsewhere). Positive homogeneity \(I(t f) = t I(f)\) for \(t \geq 0\) is immediate from the definition. An additive, positively homogeneous functional on the nonnegative cone extends uniquely to a linear functional on \(C_0(X)\) by writing a real function as a difference of its positive and negative parts and a complex function through real and imaginary parts; the extension is positive by construction and satisfies \(|F(g)| \leq I(|g|)\) since \(|g| \leq |g|\) places \(g\) among the competitors defining \(I(|g|)\).

A Positive Functional Comes From a Measure

The second step is the heart of the representation: a positive linear functional on \(C_0(X)\) is integration against a positive regular Borel measure. This is the classically named Riesz representation for positive functionals; its full construction of the measure is long, and we give the core idea.

Theorem: Positive Functionals are Positive Measures

Let \(X\) be a locally compact Hausdorff space and let \(I : C_0(X) \to \mathbb{C}\) be a positive bounded linear functional. Then there is a unique positive regular Borel measure \(\nu\) on \(X\) such that \[ I(f) \;=\; \int f \, d\nu \qquad \text{for every } f \in C_0(X), \] and \(\|I\| = \nu(X)\).

Proof Sketch

The measure is built outside-in, starting from open sets. For an open \(U \subseteq X\), define \[ \nu(U) \;=\; \sup\{\, I(\phi) : \phi \in C_0(X),\ 0 \leq \phi \leq 1,\ \operatorname{supp}\phi \subseteq U \,\}, \] the supremum of the functional over continuous "bump" functions trapped inside \(U\). This is monotone in \(U\) and, using that a bump subordinate to a union can be split into bumps subordinate to the pieces, countably subadditive. For an arbitrary set \(E\) one then sets \[ \nu(E) \;=\; \inf\{\, \nu(U) : U \supseteq E,\ U \text{ open} \,\}, \] an outer measure by construction. The technical core is to show that this outer measure is countably additive on the Borel sets — the Carathéodory measurability of open sets — which is where the bulk of the work lies and where the existence of continuous bumps separating compact sets from closed sets (a separation property of locally compact Hausdorff spaces) is used repeatedly. Outer regularity holds by definition; inner regularity follows because the bumps witnessing \(\nu(U)\) have compact support. Once \(\nu\) is a measure, the identity \(I(f) = \int f \, d\nu\) is verified first for \(0 \leq f \leq 1\) by sandwiching \(f\) between bumps adapted to the level sets \(\{f > t\}\) and integrating in \(t\), then for general \(f\) by linearity. Uniqueness follows because two regular Borel measures agreeing as functionals agree on open sets through the bump-supremum formula, hence on all Borel sets by outer regularity. Finally \(\|I\| = \nu(X)\): the bound \(|I(f)| \leq \nu(X)\|f\|_\infty\) comes from \(I(f) = \int f \, d\nu\), and equality is approached by bumps increasing to \(1\).

The two steps compose: an arbitrary bounded functional \(F\) yields a positive functional \(I\) with \(|F(g)| \leq I(|g|)\), and \(I\) is integration against a positive measure \(\nu\). The remaining task is to recover \(F\) itself — not just its positive envelope — as integration against a complex measure built from \(\nu\). Assembling this is the content of the representation theorem in the next section.

The Riesz Representation Theorem

Everything is now in place. The previous section produced, from a bounded functional \(F\), a positive functional \(I\) dominating it, and realized \(I\) as integration against a positive measure \(\nu\). We complete the circle by recovering \(F\) itself as integration against a complex measure, and we record the resulting identification of \(C_0(X)^*\) with \(M(X)\).

Theorem: Riesz Representation for \(C_0(X)\)

Let \(X\) be a locally compact Hausdorff space. For \(\mu \in M(X)\), let \(F_\mu \in C_0(X)^*\) be the functional \(F_\mu(f) = \int f \, d\mu\). Then the map \[ M(X) \longrightarrow C_0(X)^*, \qquad \mu \longmapsto F_\mu, \] is an isometric isomorphism: it is linear, \(\|F_\mu\| = \|\mu\|\) for every \(\mu\), and every bounded linear functional on \(C_0(X)\) equals \(F_\mu\) for a unique \(\mu \in M(X)\). In words, the dual of \(C_0(X)\) is the space of measures \(M(X)\).

Proof

Linearity of \(\mu \mapsto F_\mu\) and the isometry \(\|F_\mu\| = \|\mu\|\) were established earlier, and the isometry makes the map injective: \(F_\mu = 0\) forces \(\|\mu\| = 0\), hence \(\mu = 0\). Only surjectivity remains: given \(F \in C_0(X)^*\), we construct \(\mu \in M(X)\) with \(F = F_\mu\).

Form the positive functional \(I\) dominating \(F\), and let \(\nu\) be the positive regular Borel measure with \(I(g) = \int g \, d\nu\). The domination \(|F(g)| \leq I(|g|) = \int |g| \, d\nu\) says that \(F\), viewed on \(C_0(X)\) sitting inside \(L^1(\nu)\), is bounded for the \(L^1(\nu)\)-norm: \[ |F(g)| \;\leq\; \int |g| \, d\nu \;=\; \|g\|_{L^1(\nu)}. \] Since \(C_0(X)\) is dense in \(L^1(\nu)\) — continuous functions of compact support approximate \(L^1\) functions in mean, a consequence of the regularity of \(\nu\) — the functional \(F\) extends uniquely to a bounded linear functional on \(L^1(\nu)\) of norm at most \(1\). The dual of \(L^1\) is \(L^\infty\) (the duality of \(L^p\) spaces in the endpoint case \(p = 1\), treated on the page on dual spaces), so that extension is given by a function \(\phi \in L^\infty(\nu)\) with \(\|\phi\|_\infty \leq 1\): \[ F(g) \;=\; \int g \, \phi \, d\nu \qquad (g \in C_0(X)). \] Now define \(\mu\) by \(\mu(E) = \int_E \phi \, d\nu\), the measure with density \(\phi\) against \(\nu\). It is a complex measure, and its total variation is \(|\mu|(E) = \int_E |\phi| \, d\nu\), so \(|\mu| \leq \nu\); since \(\nu\) is a finite regular Borel measure, so is the dominated \(|\mu|\), whence \(\mu \in M(X)\). For every \(g \in C_0(X)\), \[ F_\mu(g) \;=\; \int g \, d\mu \;=\; \int g \, \phi \, d\nu \;=\; F(g), \] the middle equality being the change of variables for a density. Thus \(F = F_\mu\). Uniqueness is the injectivity already shown. Therefore \(\mu \mapsto F_\mu\) is an isometric isomorphism of \(M(X)\) onto \(C_0(X)^*\).

The harder direction was routed through the duality of \(L^p\) at \(p = 1\): the regularity of \(\nu\) makes \(C_0(X)\) dense in \(L^1(\nu)\), and that density is what lets a density \(\phi\) represent \(F\). Regularity is therefore essential to the construction, not cosmetic.

The Compact Case and Annihilators

When \(X\) is compact, \(C_0(X) = C(X)\) and the theorem reads \(C(X)^* = M(X)\): every continuous linear functional on \(C(X)\) is integration against a unique complex regular Borel measure, with the dual norm equal to the total variation. This is the form used when \(C(X)\) is the ambient algebra. In particular, if \(\mathcal{A} \subseteq C(X)\) is a closed subspace, its annihilator \[ \mathcal{A}^\perp \;=\; \{\, \varphi \in C(X)^* : \varphi(f) = 0 \text{ for all } f \in \mathcal{A} \,\} \] becomes, under the identification, the space of measures that integrate to zero against every member of \(\mathcal{A}\): \[ \mathcal{A}^\perp \;=\; \Bigl\{\, \mu \in M(X) : \int f \, d\mu = 0 \text{ for all } f \in \mathcal{A} \,\Bigr\}. \] An element of \(\mathcal{A}^\perp\) is now a concrete object — a measure on \(X\) — to which the full machinery of support, total variation, and integration applies. This is precisely what turns an abstract functional-analytic hypothesis about \(\mathcal{A}\) into a question about measures one can localize and manipulate.

The extreme points of the unit ball of \(M(X)\) make the same identification vivid. For a compact \(X\), those extreme points are exactly the unimodular point masses \(\alpha\delta_x\) with \(|\alpha| = 1\) and \(x \in X\): among all measures of total variation \(1\), the indecomposable ones are concentrated at a single point. A measure that lives on more than one point is an average of measures supported on smaller sets and so cannot be extreme, while a point mass admits no such splitting. Reading this through the Riesz isomorphism, the extreme points of the dual ball of \(C(X)\) are the scaled evaluations \(f \mapsto \alpha f(x)\) — the functionals that read off a single value. The structure of the dual ball is thereby reduced to the points of \(X\) themselves, the starting point for extracting a distinguished measure from an extremal functional and the bridge by which compactness arguments on the dual ball return statements about \(C(X)\).