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 67: Moment maps do not automatically select the frame-lock orbit.

Provenance

Preserved from interaction notebook section 67, 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.

67. Moment maps do not automatically select the frame-lock orbit

For G=diag⁡(1,−1,−1,0)G=\operatorname{diag}(1,-1,-1,0) and the coordinate family Z(t)=(cos⁡t,sin⁡t,0,0)Z(t)=(\cos t,\sin t,0,0), the exact moment map is μG=cos⁡(2t)\mu_G=\cos(2t). Calling sin⁡2t\sin^2t the physical frame-lock invariant is not justified without specifying the product-spin identification.

In the product basis used in Sections 72--92, Z(t)=∣+⟩⊗(cos⁡t∣+⟩+sin⁡t∣−⟩)Z(t)=|+\rangle\otimes(\cos t|+\rangle+\sin t|-\rangle) is a product state. Its concurrence is zero and its frame-lock invariant is s=1s=1 for every tt. Thus a maximum of μG\mu_G on this curve does not prove selection of s=0s=0.

The correct invariant fixed-lock test is (I−P∗)GqZ∗=0(I-P_*)G_qZ_*=0 at a separately selected lock ray, as developed in Sections 87--92. It gives q=1q=1 within the specified integer family and fixed-ray identification. It is a compatibility/stationarity condition, not a derivation of the locking potential or a proof of stability of the total Hamiltonian. The earlier comparison of two purported lock Hessians by a factor of four has no basis-independent physical interpretation.