Throughout we use the [0,β] conventions of Measure, Measure Space, and Probability Measure and, for functions with values in [0,β], the notion of measurability and the integral of Lebesgue Integral of a Nonnegative Measurable Function. Let R denote the family of measurable rectangles AΓB (AβF, BβG) of Product Sigma-Algebra; R is a Ο-system in the sense of Dynkin's Pi-Lambda Theorem, since (AΓB)β©(Aβ²ΓBβ²)=(Aβ©Aβ²)Γ(Bβ©Bβ²), it contains XΓY, and by definition it generates FβG (Generated Sigma-Algebra).
Step 0 (disjoint decompositions). By Ο-finiteness write X=βiβXiβ with ΞΌ(Xiβ)<β and Y=βnβYnβ with Ξ½(Ynβ)<β (i,n ranging over the natural numbers). Setting C1β=X1β, Ciβ=Xiββ(X1ββͺβ―βͺXiβ1β) and similarly DnββYnβ, we obtain pairwise disjoint sets CiββF, DnββG with βiβCiβ=X, βnβDnβ=Y, ΞΌ(Ciβ)β€ΞΌ(Xiβ)<β, Ξ½(Dnβ)β€Ξ½(Ynβ)<β (monotonicity of measures). Write Ξ½nβ(B)=Ξ½(Bβ©Dnβ), a finite measure on (Y,G).
Step 1 (sections). For EβXΓY and xβX let Exβ={yβY:(x,y)βE}. The class of E with ExββG for every x is a Ο-algebra β sections commute with complements, ((XΓY)βE)xβ=YβExβ, and with countable unions β and it contains R, since (AΓB)xβ equals B if xβA and β
otherwise. Hence it contains FβG.
Step 2 (measurability of section masses). Let Ξ½β² be any finite measure on (Y,G). We claim that for every EβFβG the real-valued function xβ¦Ξ½β²(Exβ) (bounded by Ξ½β²(Y)) is F-measurable. Let L be the class of such E. For a rectangle, Ξ½β²((AΓB)xβ)=Ξ½β²(B)1Aβ(x), a simple function; so RβL. L is a Ξ»-system: it contains XΓY (constant function Ξ½β²(Y)); for FβE both in L, Ξ½β²((EβF)xβ)=Ξ½β²(Exβ)βΞ½β²(Fxβ) by additivity and finiteness, and differences of real measurable functions are measurable, since {uβv>t}=βqβQβ({u>q}β©{v<qβt}) by density of the rationals; and for E1ββE2βββ¦ in L, Ξ½β²((βjβEjβ)xβ)=limjβΞ½β²((Ejβ)xβ) by continuity from below (write the increasing union as a disjoint union of successive differences and use countable additivity), and a nondecreasing pointwise limit of measurable functions is measurable because {supjβujβ>t}=βjβ{ujβ>t}. By Dynkin's Pi-Lambda Theorem, LβΟ(R)=FβG.
Step 3 (existence). For EβFβG define
m(E)=nβββ«XβΞ½nβ(Exβ)dΞΌ(x)Β β[0,β],
the series being the supremum of its partial sums; each integrand is a nonnegative real measurable function by Steps 1 and 2. Then m(β
)=0, and m is countably additive: if E1,E2,β¦ are pairwise disjoint, their sections are pairwise disjoint, so Ξ½nβ((βjβEj)xβ)=βjβΞ½nβ(Exjβ); interchanging the integral with this series is permitted because the partial sums are nondecreasing, finite sums pull out of the integral by claim 1 of Linearity and Monotonicity of the Lebesgue Integral, and Monotone Convergence Theorem applies; finally the resulting double series of nonnegative terms may be summed in either order, since both iterated sums equal the supremum of the sums over finite sets of index pairs (any finite set of pairs is contained in a finite rectangle of indices, and partial sums are monotone in both indices). This gives m(βjβEj)=βjβm(Ej). On rectangles,
m(AΓB)=nβββ«XβΞ½(Bβ©Dnβ)1AβdΞΌ=nββΞ½(Bβ©Dnβ)ΞΌ(A)=ΞΌ(A)Ξ½(B),
by the integral of simple functions, countable additivity of Ξ½ along the disjoint sets Bβ©Dnβ, and the [0,β] product conventions of Measure, Measure Space, and Probability Measure. So m is a measure on FβG with the required rectangle property. It is Ο-finite: the countably many rectangles CiβΓDnβ are pairwise disjoint, cover XΓY, and satisfy m(CiβΓDnβ)=ΞΌ(Ciβ)Ξ½(Dnβ)<β.
Step 4 (uniqueness). Let mβ² be any measure on FβG with mβ²(AΓB)=ΞΌ(A)Ξ½(B) for all rectangles. Fix i and n, and consider the two finite measures Eβ¦m(Eβ©(CiβΓDnβ)) and Eβ¦mβ²(Eβ©(CiβΓDnβ)) on FβG. For a rectangle E=AΓB, Eβ©(CiβΓDnβ)=(Aβ©Ciβ)Γ(Bβ©Dnβ) is again a rectangle, on which both assign ΞΌ(Aβ©Ciβ)Ξ½(Bβ©Dnβ); in particular both have total mass ΞΌ(Ciβ)Ξ½(Dnβ)<β. The class of E on which they agree contains XΓY and is closed under proper differences (additivity, finiteness) and increasing countable unions (continuity from below), i.e. it is a Ξ»-system containing R, hence equals FβG by Dynkin's Pi-Lambda Theorem. Since the sets CiβΓDnβ are pairwise disjoint with union XΓY, countable additivity gives, for every EβFβG,
m(E)=i,nββm(Eβ©(CiβΓDnβ))=i,nββmβ²(Eβ©(CiβΓDnβ))=mβ²(E),
(the double sums again ordered arbitrarily, as in Step 3). Hence the product measure exists and is unique, and ΞΌβΞ½=m is Ο-finite. β