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Exact binary circuit threshold in distinct-prime grids
Result and scope
Let , where is a finite set of distinct odd primes, and let be its standard integer column matrix. A binary circuit is a minimal nonempty support in . Call it liftable if its entire support carries a relation with coefficients over .
Theorem. Every binary circuit with at most eighteen vertices is liftable. There is an unliftable binary circuit with nineteen vertices already in .
Consequently, for every dissociated , the binary code has minimum distance at least nineteen. More generally, if the permitted primes start with , the minimum distance is at least . With fewer than three factors, this kernel is zero.
This is a proved finite-support lifting theorem, not an unbounded dissociated-coloring theorem or fixed-height focusing premise. In particular the modular kernel here is the full kernel of the reduced column matrix, not merely the reduction of the integer relation lattice on . The coordinates are the standard tensor basis, or a unimodular change of that basis, not an arbitrary integer encoding or a scaled matrix.
1. Singleton-layer descent
In a binary relation on , all layer sums in the reduced base agree. If one layer is empty, all sums vanish, so each occupied layer separately supports a relation. For a binary circuit this forces exactly one occupied layer. Such an inactive coordinate can be deleted without changing liftability. Every active coordinate of a circuit therefore occupies all layers.
Suppose a circuit has a singleton layer in an active coordinate. Every other layer is binary-independent, since a dependence in one layer would be a proper subdependence of . Its binary sum is . If , independence forces . Otherwise is a binary circuit: any proper relation would have to contain , and its difference with the full relation would be a dependence in . Its size is at most
If every such smaller circuit lifts, normalize its coefficient at to . Then each layer has a signed sum equal to the actual vector . For layers , use coefficient . Equal layer sums reconstruct a full-support ternary relation on . Thus an unliftable circuit with a singleton layer descends to a strictly smaller unliftable circuit on one fewer factor.
This descent may combine projections of points from different old layers. It does not preserve their colors under an arbitrary original coloring.
2. Two factors and the first tail bound
On , every binary kernel array has form , with . This follows directly by solving the equations on the first coordinates; the last row and column determine all entries. Choose representatives in . The integer array has the same support, entries in , and lies in the integer kernel because each whole row and column is a simplex relation. The one-factor case is immediate.
Repeated singleton descent from an unliftable circuit must therefore end at one with at least three active factors and no singleton layers. Its size is at least twice its largest active prime, hence at least . This proves the tail bound, with no statement of liftability at its endpoint.
3. A two-point reference layer over
To exclude bad circuits of size at most eighteen, choose one of smallest size. Delete its inactive coordinates. Section 1 excludes singleton layers; Section 2 forces at least three active primes. Each active prime is at most nine, so the active factors are exactly . Its seven layers over have size at least two. Some layer has size two, since otherwise the total size would be at least twenty-one. Denote this reference layer by .
Identify the fifteen base labels with the edges of , oriented from the three-vertex part to the five-vertex part. Over either or , the base kernel consists of graph gradients . In particular, a label set is binary-independent exactly when is connected: a supported nonzero gradient exists exactly when its complement is disconnected.
Every other layer is binary-independent and has the same binary sum as . We determine the possible signs for which has a representation on all of with coefficients .
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If contains both , then , by independence; both relative sign choices work.
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If contains exactly one, say , then is a binary circuit. It is a minimal cut (a bond) of the graph, whose integer cut vector is a full-support relation. This represents either sign of on , independently of the sign at . Again both relative signs work.
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Suppose . The graph is connected, and deleting leaves either two or three components. It cannot leave one: the nonzero binary cut vector on is constant on each component of its complement, but changes on .
With two components, is a bond. Its cut vector forces one relative sign at , and realizes that sign choice with coefficients everywhere on .
With three components, the edges form a tree connecting them. The binary cut labels the center component differently from both leaves. Every edge in consequently joins the center to a leaf, never the two leaves or a component to itself. For any prescribed signs at , assign integer potentials to the three components with those gradients on the tree edges. Every -edge then has gradient . Negating the gradient on gives the desired full-support representation of . Thus this case imposes no relative-sign constraint.
Only bond layers can constrain the relative sign, and their constraints have just the two possible values.
4. Incompatible constraints cost at least nineteen points
If share an endpoint, every cut containing both gives the same relative orientation. All layer constraints agree, and the signed layer sums reconstruct a ternary lift, a contradiction.
Otherwise write , , with distinct endpoints on both sides. A cut containing row vertices and column vertices on one side has size
For a bond containing these two disjoint edges, both complementary induced graphs are connected, so , . (An extreme side would be an isolated single vertex, which cannot cut both disjoint edges.)
If have opposite cut orientations, (2) is at least six: for it is , and for it is . If they have the same orientation, after exchanging the sides the two row endpoints are inside and the two column endpoints outside. Hence , , and the cut size is at least seven. These possibilities give layers of size at least four and five, respectively, after removing the reference edges.
An unliftable circuit needs both types of constraint; otherwise choose a compatible relative sign and reconstruct its lift as in Section 3. All seven layers have at least two points, and these two constrained layers therefore force
This contradicts the proposed counterexample of size at most eighteen.
5. Sharpness without a new search
Use the recorded twenty-point coefficient-two circuit. Its integer kernel has one generator with nineteen coefficients and one coefficient . Its verified unit minor gives rank nineteen also modulo two. Consequently its full binary kernel is one-dimensional, supported on exactly the nineteen odd-coefficient columns. Those nineteen columns form a binary circuit.
They are rationally independent, since they are a proper subset of the twenty-point rational circuit. In particular they admit no ternary lift. This proves sharpness. It uses the existing algebraic certificate; no prior experiment or certificate was rerun.
6. What this does and does not give the main route
For a dissociated -point set , every nonzero modular kernel word contains a binary circuit, so the theorem excludes weights below nineteen. Disjoint radius-nine Hamming balls give
On a prime tail, replace nine by . We use for . The modular nullity need not equal the rational nullity: the sharp nineteen-column example itself has rational nullity zero and modular nullity one.
For the already considered even-, -pivot mechanism, let be the integer-kernel rank and the number of nonpivot coordinates. The integral-kernel basis stays independent modulo two, while its pivot rows vanish. Its reduced code is therefore a -dimensional subcode supported on these positions, with distance at least nineteen. The corresponding form of the same Hamming bound is
This applies to dissociated subsets of the distinct-prime grids under the stated integral-pivot hypothesis. It sharpens the half-density ceiling only by lower-order terms; no high-density descent follows.
The new singleton descent is a precise recursive lifting alternative, but its conclusion is still local in support size. Hamming bounds of this form permit nullity density tending to one. No monochromatic structure is forced, and descent in a projected grid does not transfer actual colors. Thus neither the fixed-height premise nor the main unbounded-coloring theorem follows.
The singleton reduction, graph-potential sign analysis, bond-size bounds, and sharpness witness received independent internal review. No numerical search was run; internal review is not external review.