This work establishes a conditional reduction chain from a discrete ontological substrate to general relativity. The method does not assemble the Einstein field equations piece by piece; instead, it compresses the field equations into three structural properties—locality $(L)$, second-order $(O)$, and conserved source $(C')$—and then invokes the Lovelock uniqueness theorem to force them into Einstein form. The algebraic skeleton: zero-sum constraints fix codimension 1; the incidence matrix of a connected graph spans the zero-sum hyperplane and gives integer reachability; discrete Dirichlet energy is positive semidefinite with kernel the constants; continuum approximation combined with metric-volume consistency recovers the spatial metric; reversible/irreversible splitting directly gives signature $(1,m-1)$. The metric construction: closed-walk counting gives a parameter-free edge weight wᵢⱼ∝φᵢφⱼAᵢⱼ; finite truncation $k=n$ restores locality. The dimension account is the weakest link: the core postulates do not constrain dimension (proposition: for every m≥2 there exists a model satisfying the postulates); $D=4$ follows from two independent routes—physically, "propagating gravitons exist" requires the unique positive solution of D(D-3)2=2, and geometrically, the closure–motion correspondence principle B= combined with edge-transitivity uniquely selects K₄. The premises of both routes are not consequences of the core postulates; dimension is therefore a conditional input. **Keywords**: Lovelock theorem; general relativity; zero-sum constraint; discrete geometry; Hodge duality; dimension problem ---
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guobin ouyang (2026) studied this question.
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