Physical premise (IDWT): Physical spacetime has infinitely many ordinary spatial dimensions plus time. Matter occupies up to ten spatial dimensions; all remaining spatial directions are unbound for every particle. Depth counts a pattern's bound spatial involvement within that space. “Observed” and “unobserved” describe an observer's access, not different kinds of dimension. Older projective and nested-geometry calculations below retain their additional hypotheses; they do not establish a separate physical manifold or compactified direction. See spatial meaning and mathematical scope.

Summary: Research record, section 50: Conditional relative-separation theorem under two individual beam locks.

Provenance

Preserved from interaction notebook section 50, recorded 2026-09-05 and corrected 2026-09-06. Original sequence contents. This is an exploratory research record, not an independently established V2 result. Read the related later audits before using an intermediate conclusion.

50. Conditional relative-separation theorem under two individual beam locks

Consider abstract three-component vectors subject to the supplied linear constraints hi=QiTuih_i=Q_i^Tu_i, with Qi∈SO(3)Q_i\in SO(3). This is a constrained-algebra comparison, not an electron-trajectory premise.

At u1=u/2u_1=u/2, u2=−u/2u_2=-u/2, the difference is

h=h1−h2=Au,A=12(Q1T+Q2T). h=h_1-h_2=Au,\qquad A=\frac12(Q_1^T+Q_2^T).

For relative rotation angle ϕ\phi and ν=cos⁡2(ϕ/2)\nu=\cos^2(\phi/2),

σ(A)={1,ν,ν},∣h∣2=∣u∥∣2+ν∣u⊥∣2. \sigma(A)=\{1,\sqrt\nu,\sqrt\nu\},\qquad |h|^2=|u_{\parallel}|^2+\nu|u_{\perp}|^2.

Consequently ν∣u∣2≤∣h∣2≤∣u∣2\nu|u|^2\le|h|^2\le|u|^2. If ξ=(u,h)\xi=(u,h), then

(1+ν)∣u∣2≤∣ξ∣2≤2∣u∣2. (1+\nu)|u|^2\le|\xi|^2\le2|u|^2.

These bounds follow from the imposed vector constraints. They supply no physical correlation between observed and unobserved positions, and no particle encounter probability.