the overlap matrix. given two observers A and B with R^3 slices P_A and P_B, the overlap matrix O = P_A * P_B^T is a 3x3 matrix. its singular values measure the overlap between the slices.
three territories. the overlap matrix determines three regions relative to observer A:
every write involves the Knowable. the Known alone is inert: the wedge product needs a 2-plane, and an observer with fewer than 2 private dimensions cannot generate writes without using shared dimensions. measurement is inherently relational — not just because closure says so, but because the geometry forces it.
the vertical structure is a Grassmannian tangent. cross-measurement induces a vector in T_{P_A} Gr(3, d) = Hom(P_A, P_A^perp) that maps Knowable -> Unknown.
derivation: the neighbor’s write dL_B is confined to Lambda^2(P_B) (write_confined_to_slice). the cross-slice component of [dL_B, P_A] is purely off-diagonal (commutator_is_tangent): it maps range(P_A) -> ker(P_A). specifically: A’s Known is in P_B^perp (by definition), so B’s write kills it. the surviving component maps P_A intersect P_B (the Knowable) to P_A^perp intersect P_B (B’s territory within A’s Unknown).
this tangent is directional pressure from cross-measurement toward what the observer doesn’t yet occupy. each neighbor induces a different tangent direction.
the tangent is active but not followable. the observer’s position on Gr(3, d) is birth-committed and does not move within the map. the tangent contributes to dissonance that drives writes, but its effect lives in U(d)^N (state evolution), not in Gr(3, d) (slice movement). slice movement requires recommitment — outside the map.
containment is algebraically symmetric. B’s tangent on A has the same expected magnitude as A’s tangent on B (the overlap singular values are symmetric: sigma(O) = sigma(O^T)). experiential asymmetry (which observer “feels contained”) is perspectival, not algebraic.
the tangent peaks at intermediate overlap. identical slices: zero tangent (no Unknown territory to point toward). orthogonal slices: weak tangent (no Knowable channel — range(O) is thin). intermediate overlap: largest tangent magnitude. this is the coverage-interaction trade-off.
when three bubbles A, B, C have walls A-B and B-C but no wall A-C, B is a mandatory intermediary. (this is the algebraic form of the bridge architecture; see framing/vocabulary’s bridge entry — the bridge’s witness IS the line translation, which IS the mediator below.)
the mediation operator. M = O_AB * O_BC = P_A * Pi_B * P_C^T, where Pi_B = P_B^T * P_B is the projection onto B’s subspace. M is a 3x3 matrix mapping C’s R^3 -> A’s R^3, filtered through B. its singular values are the channel capacity of the membrane.
the bypass. O_AC - M = P_A * (I - Pi_B) * P_C^T is the A-C connection that does not go through B. if the bypass is zero, the membrane is complete.
the round-trip operator. R_A = M * M^T is self-adjoint on A’s R^3, describing what comes back from sending through B to C and back. its eigenvalues are the squared singular values of M.
spectral symmetry. the same eigenvalues appear from C’s side: R_C = M^T * M has the same nonzero eigenvalues as R_A (this is a general property of M * M^T and M^T * M). the eigenvectors differ — A and C see the same throughput spectrum from different directions. the membrane’s throughput is the same from both sides.
wall alignment is an irreducible triple invariant. the eigenvalues of R_A depend on both pairwise overlaps O_AB and O_BC and on how these overlaps are oriented relative to each other within B’s R^3. if the walls share principal directions within B, eigenvalues are products sigma^2{AB,i} * sigma^2{BC,i}. if misaligned, they mix. this alignment cannot be computed from pairwise overlaps alone — it requires all three slices.
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