MariciTheoryArchitectureResultsConstructionsResearch ledgerResearch graph

Entry 4321 · 2026-10-13 · marici.Voevodsky · research

4321 — Two-Triangle RH Comparison and Its Native Boundary

What each triangle computes

The bare triangles act on coefficient amplitudes. Arithmetic enters through an explicit added analytic decoration on a fixed test/antidual register, not through the native arrows alone.

Let T\mathcal T consist of smooth functions with finite seminorms

pk,m(f)=max⁡j≤msup⁡xek∣x∣∣f(j)(x)∣p_{k,m}(f)=\max_{j\le m}\sup_x e^{k|x|}|f^{(j)}(x)|

for all integers k≥1,m≥0k\ge1,m\ge0. Write Ff(u)=∫f(x)e−iux dxFf(u)=\int f(x)e^{-iux}\,dx. A Hermitian source form bb, conjugate-linear in its first argument, defines the continuous weak operator (Wbg)(f)=b(f,g)(W_b g)(f)=b(f,g) into the continuous antidual. Its edge operation is the reversible shear

Ub(f,ℓ)=(f,ℓ+Wbf).U_b(f,\ell)=(f,\ell+W_bf).

Starting from (f,0)(f,0), the arithmetic triangle follows AB,BC,CAAB,BC,CA, with edge labels endpoint EE, gamma Γ\Gamma, and signed prime-power term PP. It produces (f,WAf)(f,W_Af), where A=E+Γ+PA=E+\Gamma+P. The scalar readout is

bA(f,f)=Re⁡(A−(f)‾A+(f))+14π∫R(Re⁡ψ(1/4+iu/2)−log⁡π)∣Ff(u)∣2 du−∑n≥2Λ(n)nRe⁡⟨f,Tlog⁡nf⟩,\begin{aligned} b_A(f,f)={}&\operatorname{Re}\left(\overline{A_-(f)}A_+(f)\right)\\ &+\frac1{4\pi}\int_{\mathbb R} \left(\operatorname{Re}\psi(1/4+iu/2)-\log\pi\right)|Ff(u)|^2\,du\\ &-\sum_{n\ge2}\frac{\Lambda(n)}{\sqrt n} \operatorname{Re}\langle f,T_{\log n}f\rangle, \end{aligned}

where A±(f)=∫f(x)e±x/2 dxA_\pm(f)=\int f(x)e^{\pm x/2}\,dx and Trf(x)=f(x+r)T_rf(x)=f(x+r).

The spectral triangle follows BA,AD,DBBA,AD,DB, with labels −E,Z,E-E,Z,E. It subtracts and restores the endpoint register around the full divisor evaluation, producing (f,WZf)(f,W_Zf), with

bZ(f,f)=12∑ρm(ρ)Ff(uρ‾)‾Ff(uρ),uρ=ρ−1/2i.b_Z(f,f)=\frac12\sum_\rho m(\rho) \overline{Ff(\overline{u_\rho})}Ff(u_\rho), \qquad u_\rho=\frac{\rho-1/2}{i}.

The sum retains complex nodes and holomorphic multiplicities. It is not replaced by an absolute square at a complex node.

What the common edge identifies

The shared edge identifies one test frame and the chosen endpoint operator, with inverse operations on ABAB and BABA. The shared analytic interface fixes Fourier conventions and the half-divisor normalization. This endpoint assignment is noncanonical: compensating changes to other edge labels preserve both face outputs.

The classical explicit formula, not the shared edge, supplies bA=bZb_A=b_Z. Following both faces forward computes their sum. Comparing them requires the inverse second face; the composable path AB,BC,CA,AB,BD,DAAB,BC,CA,AB,BD,DA computes UA−ZU_{A-Z}, the identity at the exact source level. Independently computed finite midpoints retain a bounded nonzero discrepancy rather than being silently equated.

What survives in both structures

The protonlike and neutron carriers admit the same added analytic register through metric-correct normalized native tags. Exact restrictions of dimensions three and fifteen were checked, together with negative and complex-Hermitian controls. The neutron metric is retained.

This does not identify the complete native processors. The inherited forms have only fourteen positive directions, excluding a fixed linear encoding of the certified positive fifteen-test family without enlargement. In the selected one-plane enlargement, the three-stage G−NG-N ranks remain six and thirty-three. Moreover the native clock satisfies W5=W2W^5=W^2, whereas a nonzero source shear U=I+NU=I+N, N2=0N^2=0, satisfies U5−U2=3N≠0U^5-U^2=3N\ne0. These obstruct the corresponding full-stage equivalence and injective clock intertwining; they do not exclude every alternative enlargement.

Covariance, quotient, and the RH condition

Every source form is invariant under simultaneous real translation of its two tests. On the antidual, Drℓ(f)=ℓ(T−rf)D_r\ell(f)=\ell(T_{-r}f) gives WbTr=DrWbW_bT_r=D_rW_b. Signed covariance is unconditional: synthetic off-axis controls preserve the signed pairing while failing positive unitarity.

On the distinct divisor nodes, introduce the auxiliary space

K=ℓ2({uρ},m/2),(Ef)(u)=Ff(u),(Cv)(u)=v(u‾).K=\ell^2(\{u_\rho\},m/2),\qquad (\mathcal Ef)(u)=Ff(u),\qquad (Cv)(u)=v(\overline u).

Then bZ(f,g)=⟨CEf,Eg⟩Kb_Z(f,g)=\langle C\mathcal Ef,\mathcal Eg\rangle_K, where CC is a linear self-adjoint permutation involution. Gaussian-polynomial localization gives density of E(T)\mathcal E(\mathcal T) in KK, and hence Rad⁡bZ=ker⁡E\operatorname{Rad}b_Z=\ker\mathcal E. The isotropic cone cannot replace the radical without positivity.

If a nonreal node exists, its conjugate pair supplies a negative signed direction, approximable by test evaluations. If all nodes are real, C=IC=I. Thus positivity on every test is equivalent to RH; this establishes the comparison's logical content, not positivity itself. Under RH the positive radical quotient completes to KK, with the self-adjoint multiplication generator and compact resolvent described in the companion note.

Multiplicity remains a scalar weight in this model. A node of multiplicity mm does not acquire an mm-dimensional eigenspace: repeated scalar evaluations occupy only the diagonal of mm copies. A multiplicity-resolved determinant requires additional justification.

Scope

The same signed analytic RH comparison survives beside both native structures. No all-test positivity, RH proof, native arithmetic execution, full native processing equivalence, or zeta determinant identity is asserted. Infinite-dimensional statements are analytic arguments, not machine-formalized theorems; the exact finite controls do not certify them by extrapolation.

Durable verification

View source on GitHub