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PRs #151 and #153 substantially strengthen the continuum side of the x=21/4, spin-4 interpretation:
for the declared ordinary c=0, h=5/8 thermal module and repository normalization of Q4, the torus Ward/null-vector reduction gives
<Q4 phi>/<phi> = (493/96) g2(tau),
hence an exact ordinary-Q4 zero at the equianharmonic/hexagonal modulus;
more generally, a modular-scalar torus response at the hexagonal elliptic point suppresses spin 4 and spin 8 while allowing spin 12;
the fixed-defect Pell families give a clean O(1/N) approach to the elliptic point and a conditional two-sided scaled ratio tending to -2.
The remaining gap is operational rather than algebraic. The prediction artifacts currently write a latent component such as
DeltaM_H4(N,tau) = C N^(-13/8) E4(tau) G(tau),
but production observes a full matching/wrapping statistic, not DeltaM_H4 by itself. A raw residual can also contain H0, H12, nonlinear/composite, defect, logarithmic, and channel-dependent pieces. Without an explicit estimator that isolates or bounds the H4 component, an observed sign or accelerated power cannot be scored as the declared modular filter.
This issue is the theory/protocol gate before any N=418/780 or other Pell production is promoted.
Freeze a complete observable descriptor compatible with #146, including at least:
topology channel
primal/matching/even/odd combination
occupation/complement convention
orientation or embedding order
fixed-p versus intrinsic-center coordinate
raw contrast versus normalized harmonic projector
period matrices and period-basis convention
The scorer must hard-fail on a source/target semantic mismatch or apply a named exact map.
Required deliverable 2: an executable H4-isolating statistic
Choose and freeze one of the following, or an equally explicit construction.
A. Same-modulus embedding projector
For each Pell modulus, construct two or more microscopic square-lattice embeddings/regularizations with the same continuum period lattice and form a contrast whose response matrix to H0,H4,H8,H12,... is known exactly or to a declared truncation.
Required:
exact period/embedding arithmetic;
exact harmonic columns and orientation order;
proof that scalar H0 cancels in the contrast;
declared leakage coefficients for H8/H12/H16 and higher sectors;
an external bound or additional observations sufficient to control the leading leakage.
B. Multi-observable/channel projection
Construct a vector of scalar and vector-valued homology observables and derive a fixed linear combination that isolates the spin-4 response under the modular stabilizer action.
Required:
proof of the modular representation carried by every channel;
explicit projector matrix;
treatment of cross/either/both/directional maps;
no use of the target means to choose the projector.
C. Theory-derived subtraction with bounded remainder
If a direct projector is unavailable, freeze a decomposition
with nuisance amplitudes learned only from source/control data and propagated with full covariance. The resulting score must state the remainder class and sensitivity to each allowed sector.
A single raw DeltaM at one Pell geometry is not sufficient.
Required deliverable 3: exact and control gates
Before square-site Pell target data:
verify the period matrices, Smith/HNF data, torus modulus, and orientation conventions with the general-period reference/backend;
reproduce the modular-scalar or vector transformation on tiny exact tori where feasible;
test the proposed projector on an exactly critical control, preferably square-bond or a self-matching realization;
confirm that the statistic kills a deliberately injected pure H4 response at the exact hexagonal geometry in a synthetic/analytic test while retaining H12;
record the full covariance construction, including center/root recomputation inside every delete-one replicate.
Scoring hierarchy
Freeze before production:
primary structural score: H4-isolating statistic has the predicted opposite signs on the two Pell sides and the declared extra N^-1 suppression;
secondary cross-family score: covariance-aware residual for the scaled D=-2 versus D=+1 target (-2 asymptotically, or a separately frozen finite-modulus target);
tertiary model hierarchy: E4-only descendant/primary proxy versus literal ordinary-Q4 one-point shape, only if the lattice-to-CFT observable bridge justifies those finite-modulus predictions;
root view: report only as a derived correlated observable; do not count it as independent evidence from the same full curves.
Do not fit a free Pell exponent before these scores.
Interpretation gates
A pass supports the H4 modular-shape fingerprint only for the explicitly projected observable.
A raw total root behaving as L^-6 is not sufficient unless surviving scalar/H12/composite sectors are bounded.
An H12-like outcome would falsify ordinary local-Q4 closure more strongly than merely replacing H4 by a peer local field.
Failure of the projector/control gate blocks production interpretation; it does not weaken the existing square-torus norm-2/new-geometry evidence.
Priority
Theory/protocol work can proceed now, but square-site Pell production remains behind:
Trigger
PRs #151 and #153 substantially strengthen the continuum side of the
x=21/4, spin-4 interpretation:for the declared ordinary
c=0, h=5/8thermal module and repository normalization ofQ4, the torus Ward/null-vector reduction giveshence an exact ordinary-Q4 zero at the equianharmonic/hexagonal modulus;
more generally, a modular-scalar torus response at the hexagonal elliptic point suppresses spin 4 and spin 8 while allowing spin 12;
the fixed-defect Pell families give a clean
O(1/N)approach to the elliptic point and a conditional two-sided scaled ratio tending to-2.The remaining gap is operational rather than algebraic. The prediction artifacts currently write a latent component such as
but production observes a full matching/wrapping statistic, not
DeltaM_H4by itself. A raw residual can also contain H0, H12, nonlinear/composite, defect, logarithmic, and channel-dependent pieces. Without an explicit estimator that isolates or bounds the H4 component, an observed sign or accelerated power cannot be scored as the declared modular filter.This issue is the theory/protocol gate before any N=418/780 or other Pell production is promoted.
Required deliverable 1: typed observable definition
Freeze a complete observable descriptor compatible with #146, including at least:
The scorer must hard-fail on a source/target semantic mismatch or apply a named exact map.
Required deliverable 2: an executable H4-isolating statistic
Choose and freeze one of the following, or an equally explicit construction.
A. Same-modulus embedding projector
For each Pell modulus, construct two or more microscopic square-lattice embeddings/regularizations with the same continuum period lattice and form a contrast whose response matrix to
H0,H4,H8,H12,...is known exactly or to a declared truncation.Required:
B. Multi-observable/channel projection
Construct a vector of scalar and vector-valued homology observables and derive a fixed linear combination that isolates the spin-4 response under the modular stabilizer action.
Required:
C. Theory-derived subtraction with bounded remainder
If a direct projector is unavailable, freeze a decomposition
with nuisance amplitudes learned only from source/control data and propagated with full covariance. The resulting score must state the remainder class and sensitivity to each allowed sector.
A single raw
DeltaMat one Pell geometry is not sufficient.Required deliverable 3: exact and control gates
Before square-site Pell target data:
Scoring hierarchy
Freeze before production:
N^-1suppression;D=-2versusD=+1target (-2asymptotically, or a separately frozen finite-modulus target);Do not fit a free Pell exponent before these scores.
Interpretation gates
L^-6is not sufficient unless surviving scalar/H12/composite sectors are bounded.Priority
Theory/protocol work can proceed now, but square-site Pell production remains behind:
Related: #37, #57, #103, #114, #121, #138, #145, #146, PRs #151 and #153.