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Source. S. Korsky, A resolution of the de Bruijn--Erdős consecutive-gap problem, arXiv:2609.07196v2, Section 7: Theorem 7.1 (p. 13) and Lemma 7.2 (pp. 13--14) of the retained PDF, read in the canonical conversion and checked against the text layer at the displayed constants; held by its library card, Korsky 2026, resolution.

Standing. Author-recorded reconstruction of Lemma 7.2; not an independent review; changes no status and assigns no tier. Theorem 7.1 is an external input, cited by the source to G. Halász, On Roth's method in the theory of irregularities of point distributions, in Recent Progress in Analytic Number Theory, vol. 2 (Academic Press, 1981), 79--94; that paper is not held and the statement is not checked against it here.

Definitions

For a finite set P⊂[0,1]2\mathcal P\subset[0,1]^2 of MM points put

DP(u,v)=#(P∩((0,u]×(0,v]))−Muv(0≤u,v≤1);D_{\mathcal P}(u,v)=\#\bigl(\mathcal P\cap((0,u]\times(0,v])\bigr)-Muv \qquad(0\le u,v\le1);

endpoint conventions do not affect the integrals below. Points, PnP_n and Nn(⋅)N_n(\cdot) are as on the Lemma 2.1 page; only integer times occur here.

The imported input (Theorem 7.1, Halász)

There is an absolute constant cH>0c_H>0 such that every set P\mathcal P of M≥2M\ge2 points in [0,1]2[0,1]^2 satisfies

∫01 ⁣ ⁣∫01∣DP(u,v)∣ du dv ≥ cHlog⁡M.\int_0^1\!\!\int_0^1\bigl|D_{\mathcal P}(u,v)\bigr|\,du\,dv\ \ge\ c_H\sqrt{\log M}.

This is the unnormalized form of Halász's planar L1L^1 discrepancy theorem, as the source states it; the source gives no further derivation and none is supplied here.

Statement (Lemma 7.2, p. 13)

There are absolute constants c4>0c_4>0 and S0S_0 with the following property. Suppose S≥S0S\ge S_0, B≥1B\ge1, and, for all sufficiently large integers nn,

∫T∣Nn((x,x+D/n])−D∣ dx ≤ B(0≤D≤S).(7.1)\int_{\mathbb T}\Bigl|N_n\bigl((x,x+D/n]\bigr)-D\Bigr|\,dx\ \le\ B \qquad(0\le D\le S). \tag{7.1}

Then B≥c4log⁡SB\ge c_4\sqrt{\log S}.

Proof

Put L=⌊S⌋L=\lfloor S\rfloor, let n0n_0 be a threshold for (7.1), choose an integer N>max⁡(L,n0)N>\max(L,n_0), and put w=L/Nw=L/N. For a∈Ta\in\mathbb T let Ma=NN((a,a+w])M_a=N_N((a,a+w]) be the number of the first NN points in the arc of length w=L/Nw=L/N starting at aa. Applying (7.1) at n=Nn=N with D=LD=L,

∫T∣Ma−L∣ da ≤ B.(7.2)\int_{\mathbb T}|M_a-L|\,da\ \le\ B . \tag{7.2}

The planar point sets. View the oriented arc (a,a+w](a,a+w] as a copy of (0,1](0,1]. For each xi∈PN∩(a,a+w]x_i\in P_N\cap(a,a+w] form the point

(xi−aw, iN)∈(0,1]2,\Bigl(\frac{x_i-a}w,\ \frac iN\Bigr)\in(0,1]^2 ,

the first coordinate measured along the arc. Let Pa\mathcal P_a be the resulting set of MaM_a points, and define

Ga(u,v)=N⌊Nv⌋((a,a+uw])−Luv.G_a(u,v)=N_{\lfloor Nv\rfloor}\bigl((a,a+uw]\bigr)-Luv .

A point xix_i of the arc lies in the box (0,u]×(0,v](0,u]\times(0,v] exactly when xi∈(a,a+uw]x_i\in(a,a+uw] and i≤Nvi\le Nv, that is, i≤⌊Nv⌋i\le\lfloor Nv\rfloor; so, off a null set of (u,v)(u,v) caused by endpoints,

DPa(u,v)=N⌊Nv⌋((a,a+uw])−Mauv=Ga(u,v)+(L−Ma)uv.D_{\mathcal P_a}(u,v)=N_{\lfloor Nv\rfloor}\bigl((a,a+uw]\bigr)-M_auv =G_a(u,v)+(L-M_a)uv .

Lower bound from Halász. Since ∫01∫01uv du dv=1/4\int_0^1\int_0^1uv\,du\,dv=1/4, Theorem 7.1 gives, whenever Ma≥2M_a\ge2,

∥Ga∥L1([0,1]2) ≥ cHlog⁡Ma−14∣Ma−L∣.(7.3)\|G_a\|_{L^1([0,1]^2)}\ \ge\ c_H\sqrt{\log M_a}-\tfrac14|M_a-L| . \tag{7.3}

If B≥L/4B\ge L/4, then B≥c4log⁡SB\ge c_4\sqrt{\log S} for any fixed c4c_4 once S0S_0 is large, because L≥S−1L\ge S-1 grows faster than log⁡S\sqrt{\log S}; so assume B<L/4B<L/4. By Markov's inequality and (7.2), the set of aa with ∣Ma−L∣>L/2|M_a-L|>L/2 has measure at most (2/L)B<1/2(2/L)B<1/2, so

∣{a: L/2≤Ma≤3L/2}∣ ≥ 12.\bigl|\{a:\ L/2\le M_a\le3L/2\}\bigr|\ \ge\ \tfrac12 .

On this set Ma≥L/2≥2M_a\ge L/2\ge2 for L≥4L\ge4, and log⁡Ma≥log⁡(L/2)\sqrt{\log M_a}\ge\sqrt{\log(L/2)}; integrating (7.3) over it and using (7.2) for the subtracted term,

∫T∥Ga∥1 da ≥ cH2log⁡(L/2)−B4.(7.4)\int_{\mathbb T}\|G_a\|_1\,da\ \ge\ \frac{c_H}2\sqrt{\log(L/2)}-\frac B4 . \tag{7.4}

Upper bound from (7.1). Fix (u,v)(u,v) and put n=⌊Nv⌋n=\lfloor Nv\rfloor. If n≥n0n\ge n_0, set D=nuwD=nuw; then D≤Nuw=Lu≤L≤SD\le Nuw=Lu\le L\le S, the arc (a,a+uw](a,a+uw] has length uw=D/nuw=D/n, and

Ga(u,v)=(Nn((a,a+uw])−nuw)+Lu(nN−v),G_a(u,v)=\Bigl(N_n\bigl((a,a+uw]\bigr)-nuw\Bigr)+Lu\Bigl(\frac nN-v\Bigr),

because nuw=Lu⋅n/Nnuw=Lu\cdot n/N. The second term has absolute value at most Lu/N≤wLu/N\le w, since 0≤v−n/N<1/N0\le v-n/N<1/N; the integral over aa of the absolute value of the first term is at most BB by (7.1). On the strip 0≤v<n0/N0\le v<n_0/N, where n<n0n<n_0, trivially ∣Ga(u,v)∣≤n0+L|G_a(u,v)|\le n_0+L. Integrating over (u,v)(u,v) and then aa,

∫T∥Ga∥1 da ≤ B+LN+n0(n0+L)N=B+oN→∞(1),(7.5)\int_{\mathbb T}\|G_a\|_1\,da\ \le\ B+\frac LN+\frac{n_0(n_0+L)}N =B+o_{N\to\infty}(1), \tag{7.5}

with LL and n0n_0 fixed.

Conclusion. Combining (7.4) and (7.5) and letting N→∞N\to\infty,

54B ≥ cH2log⁡(L/2).\frac54B\ \ge\ \frac{c_H}2\sqrt{\log(L/2)} .

Since L=⌊S⌋L=\lfloor S\rfloor and S≥S0S\ge S_0 is large, log⁡(L/2)≥12log⁡S\log(L/2)\ge\frac12\log S, say, and B≥c4log⁡SB\ge c_4\sqrt{\log S} with an absolute c4>0c_4>0 after adjusting the constants; the case B≥L/4B\ge L/4 treated above is covered by the same c4c_4 once S0S_0 is large enough.

Role in the argument

Proposition 6.4 supplies (7.1) with B=C3AB=C_3A and S=Ar/Λ2S=\sqrt{Ar}/\Lambda^2; the Section 8 proof takes A=clog⁡rA=c\sqrt{\log r} and compares C3AC_3A with c4log⁡S≥c4(log⁡r)/3c_4\sqrt{\log S}\ge c_4\sqrt{(\log r)/3}.