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18 changes: 18 additions & 0 deletions experiments/universality/README.md
Original file line number Diff line number Diff line change
Expand Up @@ -178,6 +178,24 @@ This restricted parameter path is C1 but not C2 at zero and its two-site
observation law is singular; it supplies no generic two-parameter cusp,
Gaussian jet-law admission, numerical coupling or spatial process.

The [smooth two-control cusp population](two_parameter_cusp_population/PROOF.md)
extends the explicit surgery to a full smooth control rectangle through the
quartic contact. Uniform root and height guards give the complete critical
list and actual global H0 merger. Almost every field has zero or one finite
H0 bar, and the total probability of a bar is at most 1/5 for this rectangle.
Its leading whole-field lifetime density is asymptotic to
C_edge*ell^(-1/3), with cumulative count asymptotic to
(3/2)*C_edge*t^(2/3); these short bars approach the ordinary fold edges.
Restricted away from those edges, the quartic-tip density is exactly
C_tip*ell^(1/4), and the count exactly (4/5)*C_tip*t^(5/4), below the
stated cutoff. Contact sampling weight and stratum therefore both matter.
The independent-whole-copy PRM limit retains latent control, sign and
location marks; physical birth and cubic marks keep their shared-control
correlation. Its [review](two_parameter_cusp_population/REVIEW.md) preserves
original-source reviews and completed incorporated-source review. This is one
specified stationary law, with no generic full A3, Gaussian contact, Hk,
same-field spatial, numerical, formal or blind admission.

These conventional analytic results discharge selected-bar counting and the
leading near/far intensity composition for the stated ideal finite laws and
admitted stationary Gaussian spectral/carrier laws. Further
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