Derivation of ∥W∥∝M. Theorem 4 assumes the graviton amplitude scales linearly with
mass. This should follow from nbh = log 2(rs∕ℓP) = 1 + log 2M (Planck units), since more
bits produce more off-diagonal weight. A rigorous derivation would make Theorem 4 fully
self-contained.
Continuum limit and Einstein field equations. The discrete toy model uses conformal
metric configurations on a finite grid. The Einstein equations should emerge as the
large-deviation stationarity condition of the spectral complexity functional over metric
configurations in the continuum limit, analogous to how the Euler–Lagrange equations are
stationarity conditions of the action.
Full tensorial Riemann curvature. The decomposition in Theorem 2 applies to scalar
conformal factors, not the full rank-4 Riemann tensor in four dimensions. Extending the codec
decomposition to the full tensorial case is required for a complete derivation of GR.
Electromagnetic potential. The same flux argument applied to the photon residual of
Paper VII should give the Coulomb potential VEM(r) ∝ 1∕r. The ratio VEM∕Vgrav would
then give the ratio of electromagnetic to gravitational coupling, addressing the hierarchy
problem from within the framework.
Rigorous graviton propagator. The overlap integral in Theorem 4 is a heuristic. A
rigorous treatment requires the Green’s function for the graviton propagator in the discrete
model, from which the potential would follow without the proof-sketch caveat.