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Exact binary circuit threshold in distinct-prime grids


Result and scope

Let E=⨂p∈PSpE=\bigotimes_{p\in P}S_p, where PP is a finite set of distinct odd primes, and let AA be its standard integer column matrix. A binary circuit is a minimal nonempty support in ker⁡F2A‾\ker_{\mathbb F_2}\overline A. Call it liftable if its entire support carries a relation with coefficients ±1\pm1 over Z\mathbb Z.

Theorem. Every binary circuit with at most eighteen vertices is liftable. There is an unliftable binary circuit with nineteen vertices already in S3⊗S5⊗S7S_3\otimes S_5\otimes S_7.

Consequently, for every dissociated C⊆EC\subseteq E, the binary code ker⁡F2A‾C\ker_{\mathbb F_2}\overline A_C has minimum distance at least nineteen. More generally, if the permitted primes start with r1<r2<r3r_1<r_2<r_3, the minimum distance is at least max⁡(19,2r3)\max(19,2r_3). 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 CC. 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 B⊗SpB\otimes S_p, 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 pp layers.

Suppose a circuit DD has a singleton layer D0={a}D_0=\{a\} in an active coordinate. Every other layer DjD_j is binary-independent, since a dependence in one layer would be a proper subdependence of DD. Its binary sum is aa. If a∈Dja\in D_j, independence forces Dj={a}D_j=\{a\}. Otherwise Dj∪{a}D_j\cup\{a\} is a binary circuit: any proper relation would have to contain aa, and its difference with the full relation would be a dependence in DjD_j. Its size is at most

∣Dj∣+1≤∣D∣−p+2<∣D∣.(1)|D_j|+1\leq |D|-p+2<|D|. \tag{1}

If every such smaller circuit lifts, normalize its coefficient at aa to −1-1. Then each layer has a signed sum equal to the actual vector aa. For layers {a}\{a\}, use coefficient +1+1. Equal layer sums reconstruct a full-support ternary relation on DD. 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 Sp⊗SqS_p\otimes S_q, every binary kernel array has form ai+bja_i+b_j, with ai,bj∈F2a_i,b_j\in\mathbb F_2. This follows directly by solving the equations on the first (p−1)(q−1)(p-1)(q-1) coordinates; the last row and column determine all entries. Choose representatives in {0,1}\{0,1\}. The integer array ai−bja_i-b_j has the same support, entries in {−1,0,1}\{-1,0,1\}, 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 2r32r_3. This proves the tail bound, with no statement of liftability at its endpoint.

3. A two-point reference layer over S3⊗S5S_3\otimes S_5

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 3,5,73,5,7. Its seven layers over B=S3⊗S5B=S_3\otimes S_5 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 R={a,b}R=\{a,b\}.

Identify the fifteen base labels with the edges of K3,5K_{3,5}, oriented from the three-vertex part to the five-vertex part. Over either Q\mathbb Q or F2\mathbb F_2, the base kernel consists of graph gradients trow−tcolt_{\mathrm{row}}-t_{\mathrm{col}}. In particular, a label set DD is binary-independent exactly when K3,5∖DK_{3,5}\setminus D is connected: a supported nonzero gradient exists exactly when its complement is disconnected.

Every other layer DD is binary-independent and has the same binary sum as RR. We determine the possible signs ϵa,ϵb\epsilon_a,\epsilon_b for which ϵaa+ϵbb\epsilon_a a+\epsilon_b b has a representation on all of DD with coefficients ±1\pm1.

  • If DD contains both a,ba,b, then D=RD=R, by independence; both relative sign choices work.

  • If DD contains exactly one, say aa, then (D∖{a})∪{b}(D\setminus\{a\})\cup\{b\} is a binary circuit. It is a minimal cut (a bond) of the graph, whose integer cut vector is a full-support ±1\pm1 relation. This represents either sign of bb on D∖{a}D\setminus\{a\}, independently of the sign at aa. Again both relative signs work.

  • Suppose D∩R=∅D\cap R=\varnothing. The graph H=K3,5∖DH=K_{3,5}\setminus D is connected, and deleting a,ba,b leaves either two or three components. It cannot leave one: the nonzero binary cut vector on D∪RD\cup R is constant on each component of its complement, but changes on a,ba,b.

    With two components, D∪RD\cup R is a bond. Its cut vector forces one relative sign at a,ba,b, and realizes that sign choice with coefficients ±1\pm1 everywhere on DD.

    With three components, the edges a,ba,b form a tree connecting them. The binary cut labels the center component differently from both leaves. Every edge in DD consequently joins the center to a leaf, never the two leaves or a component to itself. For any prescribed signs at a,ba,b, assign integer potentials to the three components with those gradients on the tree edges. Every DD-edge then has gradient ±1\pm1. Negating the gradient on DD gives the desired full-support representation of ϵaa+ϵbb\epsilon_a a+\epsilon_b b. Thus this case imposes no relative-sign constraint.

Only bond layers D∪RD\cup R can constrain the relative sign, and their constraints have just the two possible values.

4. Incompatible constraints cost at least nineteen points

If a,ba,b 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 a=(u1,v1)a=(u_1,v_1), b=(u2,v2)b=(u_2,v_2), with distinct endpoints on both sides. A cut containing rr row vertices and ss column vertices on one side has size

5r+3s−2rs.(2)5r+3s-2rs. \tag{2}

For a bond containing these two disjoint edges, both complementary induced graphs are connected, so r∈{1,2}r\in\{1,2\}, 1≤s≤41\leq s\leq4. (An extreme side would be an isolated single vertex, which cannot cut both disjoint edges.)

If a,ba,b have opposite cut orientations, (2) is at least six: for r=1r=1 it is 5+s≥65+s\geq6, and for r=2r=2 it is 10−s≥610-s\geq6. If they have the same orientation, after exchanging the sides the two row endpoints are inside and the two column endpoints outside. Hence r=2r=2, s≤3s\leq3, and the cut size is at least seven. These possibilities give layers DD 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

∣Dtotal∣≥7⋅2+(4−2)+(5−2)=19.|D_{\rm total}|\geq 7\cdot2+(4-2)+(5-2)=19.

This contradicts the proposed counterexample of size at most eighteen.

Use the recorded twenty-point coefficient-two circuit. Its integer kernel has one generator with nineteen coefficients ±1\pm1 and one coefficient −2-2. 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 nn-point set CC, every nonzero modular kernel word contains a binary circuit, so the theorem excludes weights below nineteen. Disjoint radius-nine Hamming balls give

rank⁡QAC≥rank⁡F2A‾C≥log⁡2∑j=09(nj).(3)\operatorname{rank}_{\mathbb Q}A_C\geq \operatorname{rank}_{\mathbb F_2}\overline A_C \geq\log_2\sum_{j=0}^{9}\binom nj. \tag{3}

On a prime tail, replace nine by ⌊(max⁡(19,2r3)−1)/2⌋\lfloor(\max(19,2r_3)-1)/2\rfloor. We use (nj)=0\binom nj=0 for j>nj>n. 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-HH, HIH I-pivot mechanism, let kk be the integer-kernel rank and m=n−km=n-k the number of nonpivot coordinates. The integral-kernel basis stays independent modulo two, while its pivot rows vanish. Its reduced code is therefore a kk-dimensional subcode supported on these mm positions, with distance at least nineteen. The corresponding form of the same Hamming bound is

2k∑j=09(mj)≤2m.(4)2^k\sum_{j=0}^{9}\binom mj\leq2^m. \tag{4}

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.