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Shadow Theory

Section 9 4 October 2026

An earlier actual label is protected separately

Reading position 11 of 37

9 An earlier actual label is protected separately

For the full initial offset support,

λ+ta+.5/127<1.2299,λ−tb−.5/127>1.2301+.04001. \lambda_+t_a+.5/127<1.2299, \qquad \lambda_-t_b-.5/127>1.2301+.04001.

The compact comparison is therefore still in the common potential before tat_a and has completed writing at tbt_b. These guards concern a comparison support; they are not a claim that the exact clock has compact support at later times.

Before tat_a, use

F1(t,ξ,Z)=e−it/(2μ)[φ(ξ)+it2Mφ′′(ξ)]γ(Z−z0). F_1(t,\xi,Z)=e^{-it/(2\mu)} \left[\varphi(\xi)+\frac{it}{2M}\varphi''(\xi)\right]\gamma(Z-z_0).

Its residual norm is at most t∥φ′′′′∥/(4M2)t\norm{\varphi''''}/(4M^2). Both the exact common auxiliary evolution and each exact driven sector differ from F1F_1 by at most ta2∥φ′′′′∥/(8M2)t_a^2\norm{\varphi''''}/(8M^2). Therefore

ϵpre≤ta2(400000)4M−2. \epsilon_{\rm pre}\le\frac{t_a^2(400000)}{4M_-^2}.

This expansion has not discarded any exact clock tails.

Let ρr,jr\rho_r,j_r be the isolated spinor rotor current. Its initial density is 1/21/2, and circle Sobolev/energy estimates give

∥ρr∥∞≤3K/h,∥jr∥∞≤8K,∥ri′∥2≤K/h. \norm{\rho_r}_\infty\le3K/h,\quad \norm{j_r}_\infty\le8K,\quad \norm{r_i'}_2\le K/h.

Exact sector factorization bounds the pretrigger wave and its XX derivative errors by ϵpre\epsilon_{\rm pre} and (K/h)ϵpre(K/h)\epsilon_{\rm pre}. Thus

∥δjX∥1≤4hϵpre,∥δρ∥1≤3ϵpre. \norm{\delta j_X}_1\le4h\epsilon_{\rm pre},\qquad \norm{\delta\rho}_1\le3\epsilon_{\rm pre}.

The isolated lifted cumulative rank along the coupled ordinary path obeys

ρK˙=ρrjX−jrρ, \rho\dot{\mathcal K}=\rho_rj_X-j_r\rho,

including its circulation. Hence

EQVar⁡[0,ta]K≤120Kϵpre<6×10−18. \boxed{\E_Q\Var_{[0,t_a]}\mathcal K \le120K\epsilon_{\rm pre}<6\times10^{-18}.}

This is the physical clock-to-label error used in the periodic-current section. A global wave norm alone is not used as its replacement.