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Source. Jan Kristian Haugland, The minimum overlap problem revisited, arXiv:1609.08000v1 (2016), the edition identified on the source card. The note numbers no theorem; this page records its unlabelled 51-step construction, displayed on p. 2, together with the setting and the functional (1) on p. 1 and the 15-step and 19-step constructions on pp. 1–2.

Read depth. Claims checked: the setting, the functional (1), the step convention and all three constructions were read clause by clause on the print. The note gives no proof or verification of the reported values; the recomputation below is this page's own and is not independently reviewed.

Setting

For a partition of {1,2,…,2n}\{1,2,\ldots,2n\} into two disjoint sets {ai}\{a_i\} and {bj}\{b_j\} of nn elements each, let MkM_k be the number of solutions of ai−bj=ka_i-b_j=k for a fixed integer kk, and let M(n)M(n) be the minimum over all such partitions of max⁡kMk\max_kM_k (p. 1).

The note cites a result of Swinnerton-Dyer, proved in Haugland's 1996 paper (see the 1996 card): lim⁡n→∞M(n)/n\lim_{n\to\infty}M(n)/n equals the infimum, over all step functions ff on [0,2][0,2] with values in [0,1][0,1] and ∫02f(x) dx=1\int_0^2f(x)\,dx=1, of

max⁡k∫f(x)(1−f(x+k)) dx.(1)\max_k\int f(x)\bigl(1-f(x+k)\bigr)\,dx. \qquad(1)

The print leaves the range of integration in (1) unstated. This page reads it as the set of xx with both xx and x+kx+k in [0,2][0,2]; under that reading the three reported values below are reproduced.

A "step function with nn steps" means, in the note, a function constant on each interval (2i/n,2(i+1)/n)\bigl(2i/n,2(i+1)/n\bigr) for i∈{0,1,…,n−1}i\in\{0,1,\ldots,n-1\} (p. 1).

Statement

Construction (p. 2, unlabelled). Let ff be the step function with 51 steps that is symmetric about 11, that is f(x)=f(2−x)f(x)=f(2-x) for 1<x≤21<x\leq2, and that on [0,1][0,1] takes the values below, on [2i/51,2(i+1)/51)[2i/51,2(i+1)/51) for i=0,…,24i=0,\ldots,24 and on the half step [50/51,1][50/51,1].

xx inf(x)f(x)xx inf(x)f(x)
[0,10/51)[0,10/51)00[30/51,32/51)[30/51,32/51)0.54379073136755010.5437907313675501
[10/51,12/51)[10/51,12/51)0.00029386815562730.0002938681556273[32/51,34/51)[32/51,34/51)0.26796400489972960.2679640048997296
[12/51,14/51)[12/51,14/51)0.59528822239211770.5952882223921177[34/51,36/51)[34/51,36/51)0.85189546158237910.8518954615823791
[14/51,16/51)[14/51,16/51)0.78445308254843130.7844530825484313[36/51,38/51)[36/51,38/51)0.52111711569148720.5211171156914872
[16/51,18/51)[16/51,18/51)0.89500343380138420.8950034338013842[38/51,40/51)[38/51,40/51)11
[18/51,20/51)[18/51,20/51)0.05979640760067480.0597964076006748[40/51,42/51)[40/51,42/51)0.55061467900470430.5506146790047043
[20/51,22/51)[20/51,22/51)0.01896028384695920.0189602838469592[42/51,44/51)[42/51,44/51)0.90077153907969910.9007715390796991
[22/51,24/51)[22/51,24/51)0.74205016281729800.7420501628172980[44/51,46/51)[44/51,46/51)0.82290006919410860.8229000691941086
[24/51,26/51)[24/51,26/51)0.64445595885009210.6444559588500921[46/51,48/51)[46/51,48/51)0.88795417104401110.8879541710440111
[26/51,28/51)[26/51,28/51)0.35490408178447640.3549040817844764[48/51,50/51)[48/51,50/51)0.93154248783192210.9315424878319221
[28/51,30/51)[28/51,30/51)0.87624423850734780.8762442385073478[50/51,1][50/51,1]11

The note reports that this ff "yields the value 0.3809268534330870 for (1)" (p. 2, quoted), and calls it the best upper bound it found. With the cited Swinnerton-Dyer result this gives

lim⁡n→∞M(n)n≤0.3809268534330870,\lim_{n\to\infty}\frac{M(n)}{n}\leq0.3809268534330870,

improving the value 0.382002…0.382002\ldots of the 21-step function of the 1996 paper (p. 1). The abstract states the new bound as 0.380926…0.380926\ldots.

Earlier constructions in the note. A symmetric 15-step function (values displayed on p. 1) gives the value 0.381531550.38153155 for (1), "when rounded upwards" (p. 2, quoted); a symmetric 19-step function (p. 2) gives 0.3811122633161048160.381112263316104816. Both already improve on 0.382002…0.382002\ldots.

Comparison quoted by the note (p. 1). The best lower bound it cites is Moser's 4−15=0.356393…\sqrt{4-\sqrt{15}}=0.356393\ldots (1959). The note proves no lower bound and no optimality of its functions.

Verification

The note gives the step values only. A recomputation for this page, in exact rational arithmetic on the printed decimals: each of the three functions has integral exactly 11 over [0,2][0,2] and values in [0,1][0,1]. For a step function with steps of equal width ww, the integral in (1) is piecewise linear in kk with breakpoints at multiples of ww, so its maximum over kk is attained at a multiple of ww. Evaluating there gives 0.38092685343308697…0.38092685343308697\ldots for the 51-step function, 0.38111226331610481…0.38111226331610481\ldots for the 19-step function and 0.38153154824757…0.38153154824757\ldots for the 15-step function, which agree with the reported values as rounded in the print. For each function several shifts give values agreeing to many digits, so the maximum is not tied to one shift.

Dependencies

The bound on lim⁡M(n)/n\lim M(n)/n rests on the Swinnerton-Dyer characterization cited from Haugland, Advances in the minimum overlap problem, J. Number Theory 58 (1996), 71–78 (the 1996 card). Only the direction that every admissible step function bounds the limit from above is used.

Bears on

  • Problem 36: the problem asks for the optimal cc such that, for all large NN, every partition of {1,…,2N}\{1,\ldots,2N\} into two sets of size NN has a difference a−ba-b with at least cNcN solutions; that optimal constant is lim⁡M(N)/N\lim M(N)/N. The construction shows it is at most 0.38092685343308700.3809268534330870. An upper bound only; it does not determine the constant, and the problem page records later, smaller upper bounds.