Let K be a non-empty compact subset of R3. For any Borel probability measure μ on K, define the Newtonian energyI(μ)∈(0,∞] by
I(μ)=∫K∫K∣x−y∣1dμ(x)dμ(y)
and let RK be the infimum of I(μ) over all Borel probability measures μ on K. Show that there exists a Borel probability measure μ such that I(μ)=RK.
Solution.
By definition, there exists a sequence of Borel probability measures {μn}n on K such that I(μn)→RK. Viewing {μn}n⊆(C(K))∗, we find via Banach-Alaoglu a Borel probability measure μ and a subsequence {μnk}k such that for any continuous function f∈C(K),
∫Kf(x)dμn(x)n→∞∫Kf(x)dμ(x).
Next, we will show that μn⊗μn→μ⊗μ weakly on C(K×K). Notice that A={∑k=1nfk(x)gk(y)∣fk,gk∈C(K)} is closed under addition, scalar multiplication, and multiplication. It also separates points: if (x,y)=(x′,y′), say, x=x′, then x⋅1 separates them. Since 1∈A, it vanishes nowhere, so by Stone-Weierstrass, A is dense in C(K×K). Hence, given ε>0 and f∈C(K×K), there exist g,h∈C(K) such that ∥f(x,y)−g(x)h(y)∥L∞<ε. By weak convergence, if n is large enough, then
which proves the claim. To complete the proof, observe that (x,y)↦∣x−y∣1 is lower semicontinuous: it is continuous, except when x=y, where it is infinity. It is also bounded below by 0, so there exists a sequence of non-negative continuous functions {fn}n which increase to it. Thus,