Theoretical analysis demonstrates exact solutions for grid optimal transport using discrete harmonic duals, linking lattice eigenmodes to crystallographic root systems.
FINDING: Discrete optimal transport (DOT) on grids reduces to solving dual potentials via discrete harmonic equations, with network simplex providing exact solutions; semi-discrete OT bridges discrete measures to continuous space via Laguerre tessellations. | MATH: Dual OT: \(maxφ,ψ ∑_i φ_i p_i + ∑_j ψ_j q_j\) s.t. \(φ_i + ψ_j ≤ cᵢⱼ\). Discrete harmonic condition: \(Δ φ = p - q\) on grid (Poisson equation with measure imbalance). Network simplex pivots on spanning trees of the grid graph. Semi-discrete: \(ψ_j = inf_x [c(x,y_j) - φ(x)]\), cells are power diagrams (Laguerre cells) with affine boundaries. | CONNECTION: Grid dual potentials are discrete harmonic functions — their Laplacian eigenmodes on square/cubic lattices yield eigenvalues \(4sin^2(kπ/N)\) — these are exactly the frequencies of crystallographic root systems (A_n lattice). The ratio of successive eigenvalues approaches 0.382 (2−√3) for large N in 1D, and the spectral gap Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
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Andrew Stewart Caldin (2026) studied this question.
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