IndisputableMonolith.Gravity.SevenGaps.EdgeTensorSector
Packages the vertex-conformal log-strain as an ℝ-linear map from vertex potentials into edge perturbations, then proves finite-rank bounds showing that range is a proper subspace of the full edge space on a 5-periodic torus. Cited by anyone separating conformal scalar modes from shear in the weak-field gravity sector. Argument is linear-algebra bookkeeping: identify the map, compute ranks, and compare dimensions.
claimLet $L:\mathbb{R}^{n_V}\to\mathbb{R}^{n_E}$ be the real-linear conformal strain map sending a vertex potential to the edge log-strain by averaging endpoint values. Then $\operatorname{rank}(\operatorname{im} L)\le n_V$. On the 5-periodic torus one has $n_V<n_E$, hence $\operatorname{rank}(\operatorname{im} L)<\operatorname{rank}(\mathbb{R}^{n_E})$: the conformal sector is a proper subspace of edge perturbations.
background
Track 1.B of the gravity scaffold assigns one scalar potential per graph vertex and induces edge-length (log-strain) variations by averaging the two endpoint potentials. That construction is the conformal, pure-trace slice of the weak-field metric sector. Upstream TensorShearSector records the limitation: the scalar slice cannot represent pure shear and therefore cannot cover transverse-traceless gravitational-wave modes by itself.
This module isolates that conformal piece as an explicit $\mathbb{R}$-linear map from the vertex-potential space into the edge-perturbation space, and equips it with membership and rank lemmas. A concrete 5-periodic torus model supplies equalities for $n_V$ and $n_E$ so the rank comparison becomes numerical rather than schematic.
The setting is finite-dimensional real linear algebra on a discrete graph (or periodic lattice), not continuum GR. Edge perturbations are treated as vectors in $\mathbb{R}^{n_E}$; conformal ones are exactly the image of $L$.
proof idea
Definition layer first: the conformal strain is packaged as a LinearMap from vertex potentials to edge perturbations, with an apply lemma matching the endpoint-average formula. A membership iff characterizes conformal edge perturbations as exactly the range of that map.
Rank layer: finite-dimensional rank of the vertex-potential space and of the edge-perturbation space, plus the general inequality that the conformal range has rank at most $n_V$. On the 5-periodic torus, product equivalences fix $n_V$ and $n_E$, and the encoded edge space inherits the edge rank. Chaining those equalities yields range-rank $\le n_V < n_E$, hence a strict subspace inclusion.
why it matters in Recognition Science
Feeds the Seven-Gaps Campaign Ledger as an imported scoped increment: machine-checked separation of the conformal scalar slice from the residual edge (shear-capable) directions. The ledger style records what was proved in-kernel versus what remains open toward full physical closure, without flipping full-strength QGScopeAudit flags.
In the Recognition gravity program this is the discrete counterpart of splitting metric perturbations into trace and traceless pieces. Without a strict rank gap, one could not argue that Track 1.B misses TT-like modes; the torus comparison supplies that gap on a concrete finite model. It sits under the broader tensor/shear Track 1.D scaffold and supports later claims that a genuine shear sector is needed beyond pure conformal strain.
scope and limits
- Does not construct or classify pure shear or TT modes; only bounds the conformal range.
- Does not prove a continuum or continuum-limit statement; ranks are finite-graph linear algebra.
- Does not flip any full-strength QGScopeAudit closure flag in the campaign ledger.
- Does not claim the 5-periodic torus exhausts all physically relevant graphs.
- Does not derive Einstein equations or dynamical propagation from the rank gap.
used by (1)
depends on (1)
declarations in this module (57)
-
def
conformalStrainLinearMap -
theorem
conformalStrainLinearMap_apply -
theorem
isConformalEdgePerturbation_iff_mem_range -
theorem
finrank_vertexPotential -
theorem
finrank_edgePerturbation -
theorem
conformalRange_finrank_le_nV -
def
periodicEdge5EquivProd -
theorem
periodicTorus5_nV_eq -
theorem
periodicTorus5_nE_eq -
theorem
finrank_encodedEdgePerturbation5 -
theorem
periodicTorus5_conformalRange_finrank_le -
theorem
periodicTorus5_conformalRange_finrank_lt_finrank_edgeSpace -
theorem
periodicTorus5_conformalRange_ne_top -
theorem
periodicTorus5_exists_not_mem_conformalRange -
theorem
periodicTorus5_exists_nonconformal -
theorem
periodicConformalLogSubspace5_endpoint_form -
theorem
periodicConformalLogSubspace5_iff_encodedConformal -
def
faceVertexA -
def
faceVertexB -
def
faceVertexC -
def
faceVertexD -
def
faceEdgeAB -
def
faceEdgeDC -
def
faceEdgeBC -
def
faceEdgeAD -
theorem
faceEdgeAB_endpoints -
theorem
faceEdgeDC_endpoints -
theorem
faceEdgeBC_endpoints -
theorem
faceEdgeAD_endpoints -
def
rectangleShearFace5 -
theorem
rectangleShearFace5_apply_AB -
theorem
rectangleShearFace5_apply_DC -
theorem
rectangleShearFace5_apply_BC -
theorem
rectangleShearFace5_apply_AD -
theorem
rectangleShearFace5_apply_of_ne -
theorem
faceEdgeAB_not_mem_rest -
theorem
faceEdgeDC_not_mem_rest -
theorem
faceEdgeBC_not_mem_rest -
theorem
periodicEdgeInnerProduct5_rectangleShearFace5_left -
theorem
rectangleShearFace5_inner_conformal_eq_zero -
theorem
rectangleShearFace5_inner_self_eq_four -
theorem
rectangleShearFace5_ne_zero -
theorem
rectangleShearFace5_nonzero_in_orthogonal_complement -
theorem
rectangleShearFace5_not_conformal_typed -
def
rectangleShearFace5Encoded -
theorem
rectangleShearFace5Encoded_not_conformal -
theorem
periodicTorus5_exists_nonconformal_constructive -
def
xUniformStrain5 -
theorem
xUniformStrain5_apply_AB -
theorem
xUniformStrain5_apply_DC -
theorem
xUniformStrain5_apply_BC -
theorem
xUniformStrain5_apply_AD -
theorem
xUniformStrain5_not_conformal_typed -
theorem
xUniformStrain5Encoded_not_conformal -
theorem
rectangleShearFace5_inner_xUniformStrain5 -
theorem
xUniformStrain5_nonzero_orthogonal_component -
theorem
periodicTorus5_edge_tensor_sector_beyond_conformal