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Retain BB, SS, Ut=I+tSU_t=I+tS, β\beta, and Φt\Phi_t from [[additive_combinatorics/adamczewski_2026_erdos1/lemma_5_1|Lemma 5.1]], with t∈Zt\in\mathbb Z. Both UtU_t and β\beta are integer unimodular automorphisms.

Exact kernel

Let e0e_0 be the first standard basis vector and define the integer row vector

(a0(t),…,an(t))=e0TUt−1β−1.(1)(a_0(t),\ldots,a_n(t)) =e_0^TU_t^{-1}\beta^{-1}. \tag{1}

The inverses are integral: Ut−1U_t^{-1} is the finite geometric series in the nilpotent matrix −tS-tS, and

β−1(y0,…,yn)=(y0,…,yn−1,y0+⋯+yn).\beta^{-1}(y_0,\ldots,y_n) =(y_0,\ldots,y_{n-1},y_0+\cdots+y_n).

For x∈Zn+1x\in\mathbb Z^{n+1}, equation (1) gives

∑i=0nai(t)xi=0  ⟺  Ut−1β−1x∈{0}×Zn  ⟺  x=Φt(z) for some z∈Zn.(2)\sum_{i=0}^na_i(t)x_i=0 \iff U_t^{-1}\beta^{-1}x\in\{0\}\times\mathbb Z^n \iff x=\Phi_t(z)\text{ for some }z\in\mathbb Z^n. \tag{2}

Thus the perturbed rank-nn lattice is exactly the integer kernel of this linear form; no saturation assertion is left implicit.

Asymptotic sign and size

For each ii, the coefficient ai(t)a_i(t) is the first coordinate of the solution to

Utx=β−1ei.U_tx=\beta^{-1}e_i.

By Cramer's rule and det⁡Ut=1\det U_t=1, ai(t)a_i(t) equals the determinant of the matrix that agrees with UtU_t except for its first column, which is β−1ei\beta^{-1}e_i. Scaling the last nn columns by t−1t^{-1} multiplies it by t−nt^{-n}; the first column is unchanged, while each of the other columns becomes

t−1ej+Sj⟶Sj.t^{-1}e_j+S_j\longrightarrow S_j.

The last coordinate of every β−1ei\beta^{-1}e_i is 11. The last row of SS is zero, and the minor in its first nn rows and last nn columns is BB. Expansion along the last row therefore yields

ai(t)tn⟶(−1)ndet⁡B=D(0≤i≤n).(3)\frac{a_i(t)}{t^n}\longrightarrow(-1)^n\det B=D \qquad(0\leq i\leq n). \tag{3}

Here the sign normalization of the [[additive_combinatorics/adamczewski_2026_erdos1/lattice_reduction|triangular basis]] makes D>0D>0.

For positive integers ss, put

ts=2s+EB.t_s=2^s+E_B.

For each of the finitely many indices ii,

ai(ts)(2s)n=ai(ts)tsn(1+EB2s)n⟶D.(4)\frac{a_i(t_s)}{(2^s)^n} =\frac{a_i(t_s)}{t_s^n} \left(1+\frac{E_B}{2^s}\right)^n \longrightarrow D. \tag{4}

Consequently one can choose a single sufficiently large ss such that, simultaneously for every 0≤i≤n0\leq i\leq n,

0<ai(ts)≤2D(2s)n.(5)0<a_i(t_s)\leq2D(2^s)^n. \tag{5}

This direct normalization by (2s)n(2^s)^n is what gives the exact later bound; an estimate only in terms of tsnt_s^n would not by itself imply (5).

Finally take R=2rR=2^r and q0=2s+rq_0=2^{s+r}. Then

(ts−EB)R=2s2r=q0,(t_s-E_B)R=2^s2^r=q_0,

so [[additive_combinatorics/adamczewski_2026_erdos1/proposition_5_2|Proposition 5.2]] applies.

Source and dependencies

An explanation of the proof of Erdős Problem 1, preliminary exposition with no named author (erdosproblems.com, 2026), §6, equations (20)–(24), pp. 7–8. The edition read is named on the source card. The direct row-vector definition in (1), the first-column Cramer determinant, and the uniform finite-index limit in (4) spell out the source's normal-vector argument.

Bears on. #1.