Measurable Hall theorem 2026-10-05
For finitely many Lebesgue measurable sets and nonnegative demands , pairwise disjoint measurable subsets with exist exactly when for every index subset . Necessity is additivity and monotonicity of Lebesgue measure. For sufficiency, partition the set union into membership cells , send flow from a source through demand vertices to cells with , then to a sink. Source capacities are , cell capacities are , and intermediate capacities are . Every cut of a flow network has capacity at least by the assumed inequalities. The max-flow min-cut theorem provides the allocations, and divisibility of Lebesgue measure turns each cell allocation into disjoint pieces. If , all can simply be empty.
Write and let denote Lebesgue measure. Necessity follows from measure additivity and monotonicity: the pairwise disjoint Lebesgue measurable sets give
For sufficiency, form the finite measurable partition into membership cells
These Lebesgue measurable sets are pairwise disjoint, and . Empty cells may be retained. Construct a flow network with a source, one vertex for each index , one vertex for each cell , and a sink. Give the source-to- edge capacity , the -to- edge capacity whenever , and the -to-sink edge capacity .
Consider any cut of a flow network, and let be its index vertices on the source side. If an index-to-cell edge crosses the cut of a flow network, its capacity alone is . Otherwise every cell with lies on the source side, so the cut of a flow network has capacity at least
The cut immediately after the source has capacity . The max-flow min-cut theorem, valid for finite flow networks with real capacities, therefore supplies a flow of value . Its cell allocations satisfy
It remains to convert these numbers into Lebesgue measurable sets; this uses divisibility of Lebesgue measure. Indeed, for any Lebesgue measurable set , the function satisfies , and . Thus it has Lipschitz continuity, and the intermediate value theorem supplies a measurable subset of of any prescribed measure between and . Successively apply this to the remaining portion of each , choosing disjoint pieces of measure ; choose the empty set when . Then
This proves the measurable Hall theorem. The splitting step is essential: an arbitrary measure with an atom of a measure would not support the same conclusion. Here inclusion allows equality; even if strict inclusion is required, deleting one point of each nonempty from every preserves all measures and ensures .