
This work establishes an exact continuum scaling law for the Laplacian norm of a Gaussian test field in n spatial dimensions, ||Δψ_λ||²_{L²} = C_n × λ^(4−n),where C_n = n(n+2) × (π/2)^(n/2) × σ^(n−4) and connects it to a general instability mechanism in wave-like systems with curvature–feedback coupling.The result implies that stable, self-localized waves in infinite flat space are only possible for n ≤ 3, providing a natural mathematical bound on the number of large, continuous spatial dimensions. The analysis combines: Exact analytic integration in the continuum to confirm the scaling exponent 4−n. Numerical spectral simulations in 2D, 3D, and 4D to validate the scaling law and identify finite-domain artifacts. A discussion of physical implications for higher-dimensional field theories, extra-dimensional models, and confinement stability. Keywords: spatial dimension bound, Laplacian scaling, Gaussian field, curvature–feedback instability, continuum PDE, quantum field theory constraints, extra dimensions. Notes: The scaling law matches heuristic predictions from the six-mechanism collapse proof in the main text. A caution on numerical artifacts for n=4 periodic domains is included, along with the closed-form constants C_n for direct verification.
Gaussian field, spatial dimension bound, Extra Dimensions, Quantum Field Theory Constraints, Continuim PDE, Laplacian scaling, Curvature-feedback instability
Gaussian field, spatial dimension bound, Extra Dimensions, Quantum Field Theory Constraints, Continuim PDE, Laplacian scaling, Curvature-feedback instability
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