Kβ Universality Across q-State Systems
Kβ Universality Across q-State Systems
Published: DOI 10.5281/zenodo.23640792 Companion to: [[connectivity-scaling-law]] (DOI 10.5281/zenodo.23529072)
The result
The spectral efficiency formula and its absolute baseline are universal across q-state systems in the sopfr formulation:
c(d) = d Β· sin(Ο/d) / (2(dβ1)) [substrate-independent]
Kβ = ΟΒ²/12 = ΞΆ(2)/2 [universal baseline]
Numerically confirmed for q β {2, 3, 5, 6, 7, 10} at N = 200,000: K_q = Kβ to within 0.05% in all cases. The correction is analytically O(1/N) β 0 as N β β.
The q-restricted function
For each positive integer q, the q-restricted sum-of-prime-factors function is:
qsopfr_q(n) = Ξ£_{p coprime to q, p^a β₯ n} a Β· p
This is [[sopfr-binding-energy]] restricted to primes that do not divide q. Primes dividing q are excluded because they create degenerate interactions in a q-state system (their period divides q, producing no new information).
Ramanujan coefficient: For prime d = p coprime to q, the coefficient is p/(pβ1) β the same as for unrestricted sopfr. For prime d = p dividing q, the coefficient is 0. Excluded primes carry no Ramanujan spectral content.
Why K_q = Kβ for all q
The alternating spectral sum is dominated by large primes. Any fixed q has only finitely many prime divisors. Large primes (p β« q) are almost all coprime to q. Excluding the finitely many primes that divide q removes an O(N) contribution from a sum that scales as O(NΒ²/lnN). The correction therefore vanishes:
|S(N) β S_q(N)| = O(N) = o(NΒ²/ln N)
and so K_q β Kβ as N β β.
Physical reading: The spectral baseline is set by the distribution of large primes, not by the state count q. Whether the hardware uses binary pbits (q=2), ternary trits (q=3), or any higher-dimensional state space, the same prime spectral structure governs the efficiency at each connectivity degree d.
Substrate independence
The corollary follows directly: the formula c(d) = dΒ·sin(Ο/d)/(2(dβ1)) is substrate-independent. It applies to:
- Binary pbits (q=2): the Extropic Z1 at degree d=16 gives 1/c(16) = 9.6 β 10Γ FLOPs penalty
- Ternary trits (q=3): same formula, same efficiency ratios
- Any q-state clock model in the sopfr formulation: same formula, same Kβ baseline
This means the [[thermodynamic-computing-membrane]] analysis and the [[auditory-system-prime-resonance]] prediction both hold regardless of the specific state-space dimensionality of the underlying hardware or biological system.
What genuine c(d,q) would require
A formula that genuinely varies with q β where different state counts produce different spectral baselines β requires starting from the q-state Hamiltonian directly:
E_q = βJ Ξ£_{<i,j>} cos(2Ο(s_i β s_j)/q)
The path from this Hamiltonian to spectral constants leads to Dirichlet L-functions L(2, Ο_q) for characters Ο of Z/qZ:
- q=2: L(2, Ο_trivial) = ΟΒ²/6, Kβ = ΟΒ²/12
- q=3: L(2, Οβ) β 0.7813 (OEIS A086724)
- General q: K_q^{Hamiltonian} = L(2, Ο_q^{principal}) / (normalization)
This derivation β connecting the q-state Hamiltonian to spectral constants via Dirichlet characters β is the remaining open problem for the c(d,q) programme.
ONM reading
In the ONM framework, the universality of Kβ = ΟΒ²/12 across q-state systems reflects a deeper property: prime structure is substrate-independent. The primes do not care whether the state space has 2, 3, or q levels. They impose the same spectral skeleton regardless.
The q-state extension changes the SHAPE of possible states (more options per node) but not the DISTRIBUTION of prime-indexed spectral weights. The membrane tax c(d) is the same tax whether paid in binary currency or q-ary currency.
See also
- [[connectivity-scaling-law]] β the binary formula and its Extropic Z1 verification
- [[tusk-series]] β the spectral framework from which c(d) is derived
- [[thermodynamic-computing-membrane]] β hardware application
- [[auditory-system-prime-resonance]] β biological application (cochlear hair cells)
- [[prime-limit-consonance]] β musical application (same spectral hierarchy)
- [[orbital-prime-resonance]] β orbital mechanics application