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Structural Selection
eq:AAA_divJ_approx0

Equation AAA_divJ_approx0

CD[Ψ]=1J(x,t)0for xD.C_D[\Psi]=1 \quad\Longrightarrow\quad \nabla\cdot \mathbf{J}(\mathbf{x},t) \approx 0 \quad \text{for }\mathbf{x}\in D.

Source

Appendix AAA — Magnetism as a Consequence of Historical Matter ClosureGravity as a Temporally Closed Dynamical Phase

Gravity as a Temporally Closed Dynamical Phase/51_ppendix AAA — Magnetism as Historical Matter Closure.tex