- The paper proves that for every odd k≥341 and 0<a<1, no nonzero polynomial with nonnegative coefficients can make (1+ax²+xᵏ)Q(x) a 0-1 polynomial.
- It replaces exponent-by-exponent Boolean continuation searches with a uniform analytic method combining first-zero reduction, negative-binomial packets, exact strict log-concavity, and theta-kernel limits.
- The proof establishes a rigid pre-zero coefficient profile and then uses deterministic continuation to derive a negative terminal coefficient, while leaving odd exponents 13≤k≤339 and broader factor families open.
The problem and its background
The unfair $0$--$1$ polynomial conjecture (Problem 28 in Ben Green's list) asks whether a factorization of a polynomial C(x) with coefficients in {0,1} into monic polynomials with nonnegative real coefficients must already be a factorization into $0$--$1$ polynomials. Equivalently, a uniform finitely supported distribution on Z cannot be a convolution of two nonuniform finitely supported probability distributions.
The paper studies the trinomial test family
Pk,a(x)=1+ax2+xk,0<a<1, k odd,
and proves that for every odd k≥341 there is no nonzero polynomial Q with nonnegative coefficients such that $1$0 has all coefficients in $1$1. This is the first uniform-in-$1$2 result for this family. Prior work covered only individual exponents: Ghidelli settled $1$3 via forced recurrences, resultants, and numerical analysis; Hare's computational framework eliminated all but $1$4 of $1$5 candidate factor patterns up to degree $1$6; and the author's earlier work handled $1$7 by finite spectral boxes and exact Farkas certificates. Those methods scale poorly: characteristic roots become crowded, retained-mode boxes grow with $1$8, and continuation trees deepen rather than shrink. The present proof abandons both strategies in favor of an analytic, global argument that does not enumerate Boolean continuations at all.
The first-zero reduction
Writing $1$9 for the product digits and assuming C(x)0, the initial forcing lemma shows all odd coefficients vanish below C(x)1, even coefficients equal alternating geometric sums, and C(x)2. Letting C(x)3 be the first index C(x)4 with C(x)5, the cofactor coincides before C(x)6 with a forced sequence C(x)7 defined by a linear recurrence, and nonnegativity forces three summands to vanish simultaneously:
C(x)8
These two "anchor" equations convert a Boolean continuation problem into two exact constraints on one analytic sequence. A short argument also gives the uniform bound C(x)9. In canonical block coordinates {0,1}0, the key parameter is {0,1}1, together with the packet variance {0,1}2 and image spacing {0,1}3.
The negative-binomial packet and exact log-concavity
The generating function of the forced sequence,
{0,1}4
admits an exact decomposition into truncated sums {0,1}5 over packet images indexed by {0,1}6. Subtracting the full sum {0,1}7 isolates remainders {0,1}8 with a one-sign integral representation, so their absolute values {0,1}9 satisfy the adjunction $0$0 where $0$1 is an unnormalized negative-binomial mass with mode near $0$2. A binomial-expectation identity for the correction factor $0$3 yields the paper's principal rigidity tool:
Exact strict log-concavity. For every $0$4, $0$5, and interior $0$6, the ratios $0$7 strictly decrease with $0$8.
This holds for all parameters, not asymptotically, and drives the entire isolated-regime argument: pinning the anchor-adjacent ratio near $0$9 via the two anchor equations and the exact seam identity forces quantitative loss at every neighboring sample.
Regime decomposition of the proof
The proof splits according to $1$0 and $1$1, and each regime is closed differently.
Compact range ($1$2). Here the stationary term matters. A limiting block profile $1$3 approximates the actual coefficients to within $1$4, boundary coordinates are excluded exactly, and a Pascal-type relation reduces the two anchors to the algebraic system $1$5 plus one additional equation. A finite certificate — $1$6 candidate pairs filtered by exact integer arithmetic, directed interval evaluation giving residual separation above $1$7, and an independent modular gcd check modulo $1$8 — excludes this range entirely. This is the only finite search in the paper.
Isolated packets ($1$9, and later Z0). Dominant-image reindexing locates the packet image nearest its mode; remote images are suppressed because they begin more than six standard deviations away (Z1 in the finite strip). A coarse bootstrap using nine explicit envelope factors proves Z2 without any search over packet indices. The seam identity then pins the dominant ratio Z3 to within Z4 of Z5, and strict log-concavity converts this into curvature losses exceeding Z6. Every non-anchor coefficient in the last pre-zero cycle is thereby confined to Z7, with the adjacent sample satisfying Z8.
Spectral bootstrap (Z9). Before any theta approximation is used — deliberately, to avoid circularity — a sparse spectral projection onto a characteristic root of Pk,a(x)=1+ax2+xk,0<a<1, k odd,0 near Pk,a(x)=1+ax2+xk,0<a<1, k odd,1 proves the striking estimate
Pk,a(x)=1+ax2+xk,0<a<1, k odd,2
This exploits sparsity of Pk,a(x)=1+ax2+xk,0<a<1, k odd,3: the Lagrange projector has Pk,a(x)=1+ax2+xk,0<a<1, k odd,4 norm below Pk,a(x)=1+ax2+xk,0<a<1, k odd,5 uniformly, and the residue coefficient is bounded below by Pk,a(x)=1+ax2+xk,0<a<1, k odd,6. Combined with modal-amplitude bounds when Pk,a(x)=1+ax2+xk,0<a<1, k odd,7, the exponential smallness holds throughout the large-parameter range. Its logical role is essential: after it, changing the packet index from Pk,a(x)=1+ax2+xk,0<a<1, k odd,8 to Pk,a(x)=1+ax2+xk,0<a<1, k odd,9 alters the normalized profile by less than k≥3410, legitimizing "freezing" the slowly varying packet parameter.
Overlapping regime (k≥3411): the theta kernel. With k≥3412 exponentially small, the antiperiodic cyclic packet admits a parameter-uniform k≥3413 local limit:
k≥3414
Up to normalization this is the time-one Dirichlet heat kernel on k≥3415; the Jacobi theta product formula gives the sharp uniform curvature bound k≥3416 on the positive hump. Anchor saturation (which requires no log-concavity assumption) places both zeros high on the hump (k≥3417), adjacent-anchor matching makes their log-heights agree to k≥3418, and a discrete extraction lemma converts strong concavity into a lattice loss k≥3419 dominating the exponentially small error budget. Again every non-anchor coefficient lands in Q0 and Q1.
First-harmonic regime (Q2). In the heat-kernel picture this is ground-state dominance: an exact multiplier analysis shows the third harmonic is relatively smaller than Q3 and higher harmonics contribute below Q4 in relative Q5. The frozen profile becomes a cosine with curvature Q6 up to negligible perturbation, and the same corollary applies with enormous margin.
All four regimes converge on the common pre-zero interior profile: Q7, Q8, Q9 for $1$00, and $1$01.
Post-zero determinism and the terminal contradiction
A notable structural point is that once the static pre-zero profile holds, no branching remains: a short positivity induction forces all product digits through degree $1$02 to equal $1$03 ("no-explosion"). Under this continuation, two exact identities give
$1$04
and since $1$05 implies $1$06, the coefficient $1$07 is negative — contradicting nonnegativity of $1$08. Thus the hard part is genuinely the global pre-zero shape, not the post-zero Boolean tree.
Computer assistance and verification
The numerical content is deliberately minimal and structured: one finite algebraic certificate for the compact range (interval arithmetic plus an independent modular check), and outward-rounded scalar bounds elsewhere — seven subinterval bounds for the modal-product inequality, moment and tail constants for the $1$09 transfer, cross-image envelope majorants. Accompanying verifier archives record software versions, hashes, and margins. No step enumerates continuation trees whose depth grows with $1$10; the cutoff $1$11 reflects nonoptimized constants in regime passage, not intrinsic significance.
Limitations and open questions
Several boundaries of the result deserve emphasis. First, the theorem covers only $1$12; the cases $1$13 remain open, and the small-case machinery does not obviously extend to them. Second, the restriction to the exponent $1$14 is partly technical: the author remarks that the argument appears to use separation of delays rather than the special value $1$15, and conjectures analogous results for $1$16 with $1$17 fixed and $1$18 sufficiently large, but notes that interactions among $1$19 residue classes pose real difficulties that are not pursued. Third, the compact-range exclusion depends on computer-assisted certificates whose reproducibility rests on the archived verifiers. Finally, the author explicitly cautions against reading the result as evidence that the full conjecture is computationally accessible: for general factors with several interacting delay directions, neither exact log-concavity nor a scalar theta kernel should be expected automatically. Whether any analogue of the one-dimensional packet structure exists beyond three-term factors is left open.
Conclusion
The paper proves that the trinomial $1$20 admits no unfair factorization for all odd $1$21 and all $1$22, replacing per-exponent combinatorial computations with a uniform analytic argument built on an exact negative-binomial decomposition, strict log-concavity, a sparse spectral bootstrap driving $1$23 exponentially small, and a theta-kernel local limit identifiable with a midpoint Dirichlet heat kernel. The reduction of the entire difficulty to a static pre-zero profile — after which a deterministic continuation yields an exact terminal contradiction — suggests that for this family the crowded spectrum is best understood as a single physical-space object rather than a collection of nearly dominant modes.