Hecke-Regge Spectral Map

This note tests the next conjectural bridge step after near-diagonalization: whether the matched cotangent eigenvalues mu_i are approximately a simple scalar function of the matched centered-Hecke eigenvalues lambda_i.

For each level:

  1. build the cumulative Hecke operator set
  2. form B = J G J
  3. build L_cot(sqrt(D))
  4. match eigenspaces by maximum overlap
  5. fit the matched pairs (lambda_i, mu_i) with several one-parameter or low-parameter models

Models tested:

Local comparison: 43, 67, 163

level best fit rel. error next best next error
43 rational_11 0.000000 affine 0.127282
67 rational_11 0.046187 inverse_power 0.139191
163 rational_11 0.051635 inverse_power 0.130101

Full seven-operator cumulative levels

level best fit rel. error next best next error
163 rational_11 0.051635 inverse_power 0.130101
167 rational_11 0.033380 inverse_power 0.114459
173 rational_11 0.032869 inverse_power 0.089317
179 rational_11 0.037633 inverse_power 0.134067
181 rational_11 0.054411 inverse_power 0.111952
191 rational_11 0.022931 inverse_power 0.079568
193 rational_11 0.064548 inverse_power 0.207598
197 rational_11 0.014911 inverse_power 0.067821
199 rational_11 0.027505 inverse_power 0.064387

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Honest conclusion

The numerical bridge is stronger than mere commutator smallness: after overlap-matching eigenspaces, L_cot looks like a decreasing nonlinear spectral transform of B. But the fit is not exact, and the currently best low-complexity model is rational rather than affine.

So the plausible next conjecture is not L_cot = G, nor even L_cot ≈ a B + b I, but rather:

L_cot|_(1^⊥) ≈ f(B|_(1^⊥))

for a monotone decreasing scalar function f, with the rational (1,1) family as the current leading ansatz.