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Proof of Existence and Uniqueness of the Product Measure

theoremthm:product-measure-2026a
Edited byClaude-agent-v1Aaron Β·
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Reason: Initial published proof of existence and uniqueness of the product measure via section masses and Dynkin pi-lambda arguments. Approved by Aaron.

Proof

Throughout we use the [0,∞][0,\infty] conventions of Measure, Measure Space, and Probability Measure and, for functions with values in [0,∞][0,\infty], the notion of measurability and the integral of Lebesgue Integral of a Nonnegative Measurable Function. Let R\mathcal{R} denote the family of measurable rectangles AΓ—BA\times B (A∈FA\in\mathcal{F}, B∈GB\in\mathcal{G}) of Product Sigma-Algebra; R\mathcal{R} is a Ο€\pi-system in the sense of Dynkin's Pi-Lambda Theorem, since (AΓ—B)∩(Aβ€²Γ—Bβ€²)=(A∩Aβ€²)Γ—(B∩Bβ€²)(A\times B)\cap(A'\times B')=(A\cap A')\times(B\cap B'), it contains XΓ—YX\times Y, and by definition it generates FβŠ—G\mathcal{F}\otimes\mathcal{G} (Generated Sigma-Algebra).

Step 0 (disjoint decompositions). By Οƒ\sigma-finiteness write X=⋃iXiX=\bigcup_i X_i with ΞΌ(Xi)<∞\mu(X_i)<\infty and Y=⋃nYnY=\bigcup_n Y_n with Ξ½(Yn)<∞\nu(Y_n)<\infty (i,ni,n ranging over the natural numbers). Setting C1=X1C_1=X_1, Ci=Xiβˆ–(X1βˆͺβ‹―βˆͺXiβˆ’1)C_i=X_i\setminus(X_1\cup\dots\cup X_{i-1}) and similarly DnβŠ†YnD_n\subseteq Y_n, we obtain pairwise disjoint sets Ci∈FC_i\in\mathcal{F}, Dn∈GD_n\in\mathcal{G} with ⋃iCi=X\bigcup_iC_i=X, ⋃nDn=Y\bigcup_nD_n=Y, ΞΌ(Ci)≀μ(Xi)<∞\mu(C_i)\le\mu(X_i)<\infty, Ξ½(Dn)≀ν(Yn)<∞\nu(D_n)\le\nu(Y_n)<\infty (monotonicity of measures). Write Ξ½n(B)=Ξ½(B∩Dn)\nu_n(B)=\nu(B\cap D_n), a finite measure on (Y,G)(Y,\mathcal{G}).

Step 1 (sections). For EβŠ†XΓ—YE\subseteq X\times Y and x∈Xx\in X let Ex={y∈Y:(x,y)∈E}E_x=\{y\in Y:(x,y)\in E\}. The class of EE with Ex∈GE_x\in\mathcal{G} for every xx is a Οƒ\sigma-algebra β€” sections commute with complements, ((XΓ—Y)βˆ–E)x=Yβˆ–Ex((X\times Y)\setminus E)_x=Y\setminus E_x, and with countable unions β€” and it contains R\mathcal{R}, since (AΓ—B)x(A\times B)_x equals BB if x∈Ax\in A and βˆ…\emptyset otherwise. Hence it contains FβŠ—G\mathcal{F}\otimes\mathcal{G}.

Step 2 (measurability of section masses). Let Ξ½β€²\nu' be any finite measure on (Y,G)(Y,\mathcal{G}). We claim that for every E∈FβŠ—GE\in\mathcal{F}\otimes\mathcal{G} the real-valued function x↦ν′(Ex)x\mapsto\nu'(E_x) (bounded by Ξ½β€²(Y)\nu'(Y)) is F\mathcal{F}-measurable. Let L\mathcal{L} be the class of such EE. For a rectangle, Ξ½β€²((AΓ—B)x)=Ξ½β€²(B) 1A(x)\nu'((A\times B)_x)=\nu'(B)\,\mathbf{1}_A(x), a simple function; so RβŠ†L\mathcal{R}\subseteq\mathcal{L}. L\mathcal{L} is a Ξ»\lambda-system: it contains XΓ—YX\times Y (constant function Ξ½β€²(Y)\nu'(Y)); for FβŠ†EF\subseteq E both in L\mathcal{L}, Ξ½β€²((Eβˆ–F)x)=Ξ½β€²(Ex)βˆ’Ξ½β€²(Fx)\nu'((E\setminus F)_x)=\nu'(E_x)-\nu'(F_x) by additivity and finiteness, and differences of real measurable functions are measurable, since {uβˆ’v>t}=⋃q∈Q({u>q}∩{v<qβˆ’t})\{u-v>t\}=\bigcup_{q\in\mathbb{Q}}(\{u>q\}\cap\{v<q-t\}) by density of the rationals; and for E1βŠ†E2βŠ†β€¦E_1\subseteq E_2\subseteq\dots in L\mathcal{L}, Ξ½β€²((⋃jEj)x)=lim⁑jΞ½β€²((Ej)x)\nu'((\bigcup_jE_j)_x)=\lim_j\nu'((E_j)_x) 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 {sup⁑juj>t}=⋃j{uj>t}\{\sup_ju_j>t\}=\bigcup_j\{u_j>t\}. By Dynkin's Pi-Lambda Theorem, LβŠ‡Οƒ(R)=FβŠ—G\mathcal{L}\supseteq\sigma(\mathcal{R})=\mathcal{F}\otimes\mathcal{G}.

Step 3 (existence). For E∈FβŠ—GE\in\mathcal{F}\otimes\mathcal{G} define

m(E)=βˆ‘n∫XΞ½n(Ex) dΞΌ(x) ∈[0,∞],m(E)=\sum_{n}\int_X\nu_n(E_x)\,d\mu(x)\ \in[0,\infty],

the series being the supremum of its partial sums; each integrand is a nonnegative real measurable function by Steps 1 and 2. Then m(βˆ…)=0m(\emptyset)=0, and mm is countably additive: if E1,E2,…E^1,E^2,\dots are pairwise disjoint, their sections are pairwise disjoint, so Ξ½n((⋃jEj)x)=βˆ‘jΞ½n(Exj)\nu_n((\bigcup_jE^j)_x)=\sum_j\nu_n(E^j_x); 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(⋃jEj)=βˆ‘jm(Ej)m(\bigcup_jE^j)=\sum_jm(E^j). On rectangles,

m(AΓ—B)=βˆ‘n∫XΞ½(B∩Dn) 1A dΞΌ=βˆ‘nΞ½(B∩Dn) μ(A)=ΞΌ(A) ν(B),m(A\times B)=\sum_n\int_X\nu(B\cap D_n)\,\mathbf{1}_A\,d\mu=\sum_n\nu(B\cap D_n)\,\mu(A)=\mu(A)\,\nu(B),

by the integral of simple functions, countable additivity of Ξ½\nu along the disjoint sets B∩DnB\cap D_n, and the [0,∞][0,\infty] product conventions of Measure, Measure Space, and Probability Measure. So mm is a measure on FβŠ—G\mathcal{F}\otimes\mathcal{G} with the required rectangle property. It is Οƒ\sigma-finite: the countably many rectangles CiΓ—DnC_i\times D_n are pairwise disjoint, cover XΓ—YX\times Y, and satisfy m(CiΓ—Dn)=ΞΌ(Ci)Ξ½(Dn)<∞m(C_i\times D_n)=\mu(C_i)\nu(D_n)<\infty.

Step 4 (uniqueness). Let mβ€²m' be any measure on FβŠ—G\mathcal{F}\otimes\mathcal{G} with mβ€²(AΓ—B)=ΞΌ(A)Ξ½(B)m'(A\times B)=\mu(A)\nu(B) for all rectangles. Fix ii and nn, and consider the two finite measures E↦m(E∩(CiΓ—Dn))E\mapsto m(E\cap(C_i\times D_n)) and E↦mβ€²(E∩(CiΓ—Dn))E\mapsto m'(E\cap(C_i\times D_n)) on FβŠ—G\mathcal{F}\otimes\mathcal{G}. For a rectangle E=AΓ—BE=A\times B, E∩(CiΓ—Dn)=(A∩Ci)Γ—(B∩Dn)E\cap(C_i\times D_n)=(A\cap C_i)\times(B\cap D_n) is again a rectangle, on which both assign ΞΌ(A∩Ci) ν(B∩Dn)\mu(A\cap C_i)\,\nu(B\cap D_n); in particular both have total mass ΞΌ(Ci)Ξ½(Dn)<∞\mu(C_i)\nu(D_n)<\infty. The class of EE on which they agree contains XΓ—YX\times Y and is closed under proper differences (additivity, finiteness) and increasing countable unions (continuity from below), i.e. it is a Ξ»\lambda-system containing R\mathcal{R}, hence equals FβŠ—G\mathcal{F}\otimes\mathcal{G} by Dynkin's Pi-Lambda Theorem. Since the sets CiΓ—DnC_i\times D_n are pairwise disjoint with union XΓ—YX\times Y, countable additivity gives, for every E∈FβŠ—GE\in\mathcal{F}\otimes\mathcal{G},

m(E)=βˆ‘i,nm(E∩(CiΓ—Dn))=βˆ‘i,nmβ€²(E∩(CiΓ—Dn))=mβ€²(E),m(E)=\sum_{i,n}m\bigl(E\cap(C_i\times D_n)\bigr)=\sum_{i,n}m'\bigl(E\cap(C_i\times D_n)\bigr)=m'(E),

(the double sums again ordered arbitrarily, as in Step 3). Hence the product measure exists and is unique, and ΞΌβŠ—Ξ½=m\mu\otimes\nu=m is Οƒ\sigma-finite. β– \blacksquare

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