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Mrose 1979 untere schranken reichweiten extremalbasen fester ordnung

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equation_3: Mrose's lower bound n_2(k) >= (8/7)(k/2)^2 + O(k) for the range of a finite additive 2-basis with k positive elements, from his order-raising construction with the parameters t_2 = 3 and alpha_1 = k/7 + O(1); it gives liminf n(k)/k^2 >= 2/7 and so g(n)^2 <= (7/2 + o(1)) n for Problem 791.

satz_1: Mrose's order-raising construction: from an interval basis of order h for n_h, split into h sets each containing 0 that represent every n <= n_h with one summand from each set, and natural numbers alpha_{h+1}, t_{h+1} and an index i, it builds an interval basis of order h + 1 with the same property for an explicit range n_{h+1}; the source of the 2-basis behind equation (3).

satz_2: Mrose's lower bound for the largest range n_h(k) of an interval basis of fixed order h >= 2 with k positive elements: (8/7)^{h/2}(k/h)^h + O(k^{h-1}) for even h and (32/27)(8/7)^{(h-3)/2}(k/h)^h + O(k^{h-1}) for odd h, from equations (3) and (4) and a composition theorem of the author's 1974 paper.


A. Mrose, Untere Schranken für die Reichweiten von Extremalbasen fester Ordnung, Abh. Math. Sem. Univ. Hamburg 48 (1979), no. 1, 118--124, DOI 10.1007/BF02941296; received 25 April 1975 ("Eingegangen am 25. 4. 1975", p. 124); the author at the I. Mathematisches Institut der Freien Universität Berlin (p. 124). Cited as [Mr79] on the problem page. The title reads "Lower bounds for the ranges of extremal bases of fixed order". The source read for this card is the publisher's version of record at https://doi.org/10.1007/BF02941296; no preprint or repository version is known here. The scan carries no journal header, so the volume, year and DOI come from the publisher's record; the printed page numbers 119--124 are read from the running heads, and p. 118 is the title page that precedes them. Its three references (p. 124) are the author's own 1974 paper, "Ein rekursives Konstruktionsverfahren für Abschnittsbasen", J. reine angew. Math. 271 (1974), 214--217; Rohrbach, "Ein Beitrag zur additiven Zahlentheorie", Math. Z. 42 (1937), 1--30, the origin of Problem 791's function; and Stöhr, "Gelöste und ungelöste Fragen über Basen der natürlichen Zahlenreihe I", J. reine angew. Math. 194 (1955), 40--65. None of the three is held.

The copy read for this card is the publisher's scan of the printed article: 7 pages, printed pp. 118--124 = PDF pp. 1--7 (printed p. nn is PDF p. n−117n-117), a 2008 scan (the copy's metadata names a TIFF source and an August 2008 creation date) with an OCR text layer that locates the prose and garbles nearly every formula (umlauts, subscripts, superscripts, fractions, set braces and inequality signs come out as stray letters and digits). Provenance: obtained from the publisher on 2026-09-22 as a DRM-free production PDF through the library's acquisition, from https://doi.org/10.1007/BF02941296; 236,573 bytes. No notice is printed in the copy; the publisher's article page shows "© Mathematisches Seminar der Universität Hamburg 1979", paywalled with a reprints-and-permissions link, and names no open-access or Creative Commons license (https://link.springer.com/article/10.1007/BF02941296, read 2026-10-02), every other right reserved.

Read status: claims checked for the definitions and the survey of known constants (1) and (2) with equation (3) (p. 118), the comparison with Stöhr's nk(2)n_k(2) and the statement of Satz 1 (p. 119), the order-2 construction B2B_2 with its range n2n_2 and element count k2k_2 (p. 121), the parameter choices and the displays leading to equations (3) and (4) and the statement of Satz 2 (p. 123), and equation (6) with the induction and the reference list (p. 124), each read clause by clause on the page images of PDF pp. 1, 2, 4, 6 and 7 on 2026-09-22. On 2026-10-08 the Bemerkung (p. 120), the order-3 construction B3B_3 with its range n3n_3 and count k3k_3 and the elimination of αh\alpha_h (p. 122) were also read clause by clause. The proof of Satz 1 (pp. 120--121) was read for structure only; no case of the proof was checked, and its construction was run on small parameters as a filing check (recorded on the Satz 1 page). The arithmetic from the stated parameters to the leading terms of (3) and (4) on p. 123 was followed. Nothing here is independently reviewed.

Contents

  • Definitions and survey (p. 118, page image). For natural numbers hh, kk and nn, a set BB of k+1k+1 non-negative integers 0≤bκ≤n0\le b_\kappa\le n is an Abschnittsbasis (interval basis) of order hh for nn if every non-negative integer ν≤n\nu\le n is a sum of hh elements of BB, that is, B⊂{0,1,…,n}⊂hBB\subset\{0,1,\ldots,n\}\subset hB; the largest such nn for given hh and kk is nh(k)n_h(k), and the bases attaining it are Extremalbasen. Since 0∈hB0\in hB forces 0∈B0\in B, the count kk is the number of positive elements ("B2B_2 enthält die 0 sowie höchstens k2k_2 ... positive Elemente", p. 121); Kohonen's kk for Problem 791 counts the zero, so Mrose's n2(k)n_2(k) is Kohonen's n(k+1)n(k+1), which changes no asymptotic ratio. Known lower bounds have the shape (1), nh(k)≥ch(k/h)h+O(kh−1)n_h(k)\ge c_h(k/h)^h+O(k^{h-1}), and the largest known constants are listed: c1=1c_1=1 (with equality, n1(k)=kn_1(k)=k), c2=1c_2=1 (Rohrbach [2]) and ch=(8/7)[h/3]c_h=(8/7)^{[h/3]} for h≥3h\ge3 (the author's [1]). The paper proves that (1) also holds with (2): c2=8/7c_2=8/7, c3=32/27c_3=32/27, c2η=(8/7)ηc_{2\eta}=(8/7)^\eta and c2η+1=(8/7)η−1⋅32/27c_{2\eta+1}=(8/7)^{\eta-1}\cdot32/27. The author writes that the construction behind them should also yield further sharpenings of (2) for h≥4h\ge4, at a computational cost growing quickly with hh, which the paper does not pursue. Equation (3), quoted as printed: "n2(k)≥87(k2)2+O(k)n_2(k)\ge\frac87\bigl(\frac k2\bigr)^2+O(k)".
  • Comparison with Stöhr and the statement of Satz 1 (p. 119, page image). Equation (3) shows that n2(k)n_2(k) and nk(2)n_k(2) are not asymptotically equal as k→∞k\to\infty: Stöhr [3] gives nk(2)=(k/2)2+O(k)n_k(2)=(k/2)^2+O(k), so n2(k)≥87nk(2)+O(k)n_2(k)\ge\frac87n_k(2)+O(k); whether other orders hh admit nh(k)≥γ nk(h)+O(kh−1)n_h(k)\ge\gamma\,n_k(h)+O(k^{h-1}) with some γ=γ(h)>1\gamma=\gamma(h)>1 the construction could not decide. Satz 1 is the order-raising step. Given non-empty sets A1(h),…,Ah(h)A^{(h)}_1,\ldots,A^{(h)}_h of non-negative integers with 00 in each, whose union BhB_h is an interval basis of order hh for nhn_h such that every n≤nhn\le n_h is a sum ∑ηaη\sum_\eta a_\eta with aη∈Aη(h)a_\eta\in A^{(h)}_\eta, choose natural numbers αh+1\alpha_{h+1}, th+1t_{h+1} and an index i≤hi\le h, list $A^{(h)}i={0=a^{(0)}i<a^{(1)}i<\cdots< a^{(j{i,h})}i}$, and set rh=nh−max⁡j(ai(j)−ai(j−1)−1)r_h=n_h-\max_j(a^{(j)}_i-a^{(j-1)}_i-1), Di(h+1)={(αh+1+j)rh+ai(j):0≤j≤ji,h}D^{(h+1)}_i=\{(\alpha_{h+1}+j)r_h+a^{(j)}_i:0\le j\le j_{i,h}\}, $A^{(h+1)}i=({0,2\alpha{h+1}r_h,(3\alpha{h+1}+j{i,h})r_h, (4\alpha{h+1}+2j_{i,h})r_h,\ldots,(t_{h+1}\alpha_{h+1}+(t_{h+1}-2)j_{i,h})r_h} +A^{(h)}_i)\cup D^{(h+1)}_i$, Ah+1(h+1)={0,rh,2rh,…,(αh+1−1)rh}∪Di(h+1)A^{(h+1)}_{h+1}=\{0,r_h,2r_h,\ldots,(\alpha_{h+1}-1)r_h\}\cup D^{(h+1)}_i and Aj(h+1)=Aj(h)A^{(h+1)}_j=A^{(h)}_j for j≠ij\ne i. Then Bh+1=⋃jAj(h+1)B_{h+1}=\bigcup_jA^{(h+1)}_j is an interval basis of order h+1h+1 for nh+1=((th+1+1)αh+1+(th+1−1)ji,h)rh+nhn_{h+1}=((t_{h+1}+1)\alpha_{h+1}+(t_{h+1}-1)j_{i,h})r_h+n_h, with the same one-summand-per-set property.
  • Proof of Satz 1 (pp. 120--121, page images, structure only). A remark notes the overlaps Di(h+1)⊂Ai(h+1)∩Ah+1(h+1)D^{(h+1)}_i\subset A^{(h+1)}_i\cap A^{(h+1)}_{h+1} and Ai(h)∩Aj(h)⊂Ai(h+1)∩Aj(h+1)A^{(h)}_i\cap A^{(h)}_j\subset A^{(h+1)}_i\cap A^{(h+1)}_j to be taken into account when counting elements. The proof writes n≤nh+1n\le n_{h+1} as n=x+dn=x+d with xx in the multiplier set of Ai(h+1)A^{(h+1)}_i and splits on whether d≤(αh+1+ji,h)rh+nhd\le(\alpha_{h+1}+j_{i,h})r_h+n_h (Fall 1: d=ah+1+δd=a_{h+1}+\delta with ah+1∈Ah+1(h+1)a_{h+1}\in A^{(h+1)}_{h+1} and δ≤nh\delta\le n_h representable by the hypothesis, and x+ai∈Ai(h+1)x+a_i\in A^{(h+1)}_i) or not (Fall 2: then x=0x=0, n=qrh+δn=qr_h+\delta with αh+1+ji,h≤q≤2αh+1\alpha_{h+1}+j_{i,h}\le q\le2\alpha_{h+1}, and an element (αh+1+μ)rh+ai(\alpha_{h+1}+\mu)r_h+a_i of Di(h+1)D^{(h+1)}_i absorbs part of qrhqr_h).
  • The orders 2 and 3 (pp. 121--122; p. 121 on the page image, p. 122 for structure). Starting from the only order-1 basis B1=A1(1)={0,1,…,α1}B_1=A^{(1)}_1=\{0,1,\ldots,\alpha_1\} (n1=r1=j1,1=α1n_1=r_1=j_{1,1}=\alpha_1, i=1i=1), Satz 1 with parameters α2\alpha_2, t2t_2 gives the order-2 basis B2=A1(2)∪A2(2)B_2=A^{(2)}_1\cup A^{(2)}_2 with $D^{(2)}_1={\alpha_2\alpha_1,(\alpha_2+1)\alpha_1+1,\ldots, (\alpha_2+\alpha_1)\alpha_1+\alpha_1}$, A2(2)={0,α1,2α1,…,(α2−1)α1}∪D1(2)A^{(2)}_2=\{0,\alpha_1,2\alpha_1,\ldots,(\alpha_2-1)\alpha_1\}\cup D^{(2)}_1, $A^{(2)}_1=({0,2\alpha_2\alpha_1,(3\alpha_2+\alpha_1)\alpha_1, (4\alpha_2+2\alpha_1)\alpha_1,\ldots,(t_2\alpha_2+(t_2-2)\alpha_1)\alpha_1} +{0,1,2,\ldots,\alpha_1})\cup D^{(2)}_1$, of range n2=((t2+1)α2+(t2−1)α1)α1+α1n_2=((t_2+1)\alpha_2+(t_2-1)\alpha_1)\alpha_1+\alpha_1 and with at most k2=(t2+1)(α1+1)+α2−2k_2=(t_2+1)(\alpha_1+1)+\alpha_2-2 positive elements besides 00. A second application with i=2i=2 (chosen because i=1i=1 would lose a range of the order of n2n_2) and parameters α3\alpha_3, t3t_3 gives B3B_3 with $n_3=((t_3+1)\alpha_3+(t_3-1)(\alpha_1+\alpha_2)+1) ((t_2+1)\alpha_2+(t_2-1)\alpha_1)\alpha_1+\alpha_1$ and k3=t2(α1+1)+(t3+1)(α1+α2+1)+α3−3k_3=t_2(\alpha_1+1)+(t_3+1)(\alpha_1+\alpha_2+1)+\alpha_3-3. To bound nh(k)n_h(k) from below the parameters are chosen with kh=kk_h=k and nhn_h maximal; αh\alpha_h is eliminated first, giving n2=((t2+1)(k−(t2+1)(α1+1)+2)+(t2−1)α1+1)α1n_2=((t_2+1)(k-(t_2+1)(\alpha_1+1)+2)+(t_2-1)\alpha_1+1)\alpha_1 and the corresponding expression for n3n_3.
  • Parameter choices, equations (3) and (4), and Satz 2 (p. 123, page image). The remaining parameters are said to follow by the usual rules from a simple but lengthy extreme-value calculation, which the paper does not reproduce. For h=2h=2 and large kk, α1=k/7+O(1)\alpha_1=k/7+O(1) and t2=3t_2=3 give n2=(4(k−47k)+27k+O(1))(17k+O(1))=87(k2)2+O(k)n_2=(4(k-\frac47k)+\frac27k+O(1))(\frac17k+O(1))=\frac87(\frac k2)^2+O(k), whence (3): n2(k)≥87(k2)2+O(k)n_2(k)\ge\frac87(\frac k2)^2+O(k) as k→∞k\to\infty. For h=3h=3, α1=281k+O(1)\alpha_1=\frac2{81}k+O(1), α2=681k+O(1)\alpha_2=\frac6{81}k+O(1), t2=13t_2=13 and t3=3t_3=3 give n3=3227(k3)3+O(k2)n_3=\frac{32}{27}(\frac k3)^3+O(k^2), whence (4): n3(k)≥3227(k3)3+O(k2)n_3(k)\ge\frac{32}{27}(\frac k3)^3+O(k^2). Satz 2, quoted: "Für festes h≥2h\ge2 und k→∞k\to\infty gilt (5) nh(k)≥(87)h/2(kh)h+O(kh−1)n_h(k)\ge(\frac87)^{h/2}(\frac kh)^h+O(k^{h-1}) für 2∣h2\mid h, nh(k)≥3227(87)(h−3)/2(kh)h+O(kh−1)n_h(k)\ge\frac{32}{27}(\frac87)^{(h-3)/2}(\frac kh)^h+O(k^{h-1}) für 2∤h2\nmid h."
  • Proof of Satz 2 (pp. 123--124, page images). The author's [1] proved that nh1(k)≥αh1(k/h1)h1+O(kh1−1)n_{h_1}(k)\ge\alpha_{h_1}(k/h_1)^{h_1}+O(k^{h_1-1}) and nh2(k)≥αh2(k/h2)h2+O(kh2−1)n_{h_2}(k)\ge\alpha_{h_2}(k/h_2)^{h_2}+O(k^{h_2-1}) for fixed h1h_1, h2h_2 imply nh1+h2(k)≥αh1αh2(kh1+h2)h1+h2+O(kh1+h2−1)n_{h_1+h_2}(k)\ge\alpha_{h_1}\alpha_{h_2}(\frac k{h_1+h_2})^{h_1+h_2}+O(k^{h_1+h_2-1}). With h1=2h_1=2, h2=hh_2=h and (3) this is (6), nh+2(k)≥87αh(kh+2)h+2+O(kh+1)n_{h+2}(k)\ge\frac87\alpha_h(\frac k{h+2})^{h+2}+O(k^{h+1}), so (5) for h=h0h=h_0 gives (5) for h0+2h_0+2, and the cases h=2h=2 and h=3h=3 are (3) and (4). A filing observation, not a review verdict: the introduction's list (2) writes the odd-order constant as c2η+1=(8/7)η−1⋅32/27c_{2\eta+1}=(8/7)^{\eta-1}\cdot32/27 and Satz 2 writes it as 3227(8/7)(h−3)/2\frac{32}{27}(8/7)^{(h-3)/2}; with h=2η+1h=2\eta+1 these agree.
  • Literatur (p. 124, page image): the three references listed above, the received date and the author's address.

Compiled scope

The paper is compiled at statement depth on three result pages: Satz 1, the order-raising construction; Satz 2, the bound for every order h≥2h\ge2 with equation (4) as its case h=3h=3; and equation (3), the case h=2h=2 that Problem 791 consumes, read on pp. 118 and 123 with the parameters that produce it. The proof of Satz 1 was read for structure only, and its construction was run on small parameters as a filing check; the parameter optimization is not printed; the composition theorem behind Satz 2 for h≥4h\ge4 is the author's 1974 paper, not held. The arithmetic from the stated parameters to the leading terms of (3) and (4) was followed. Nothing here is independently reviewed.

Bears on. #791: equation (3) (printed p. 118, PDF p. 1, and derived on printed p. 123, PDF p. 6), "n2(k)≥87(k2)2+O(k)n_2(k)\ge\frac87\bigl(\frac k2\bigr)^2+O(k)", is the construction the site's commentary credits with the disproof of g(n)∼2n1/2g(n)\sim2n^{1/2}: it reads n2(k)≥27k2+O(k)n_2(k)\ge\frac27k^2+O(k), so lim inf⁡n(k)/k2≥2/7\liminf n(k)/k^2\ge2/7 in Kohonen's notation (the "2/7" that [Ko17] quotes for Mrose), and by the conversion written on the problem page g(n)2≤(72+o(1))ng(n)^2\le(\frac72+o(1))n, the site's "g(n)2≤72ng(n)^2\le\frac72n", whence lim sup⁡g(n)/n≤7/2<2\limsup g(n)/\sqrt n\le\sqrt{7/2}<2. The explicit basis is B2B_2 of p. 121, built by Satz 1, with t2=3t_2=3 and α1=k/7+O(1)\alpha_1=k/7+O(1); equation (3) is the case h=2h=2 of Satz 2, whose cases h≥3h\ge3 concern bases of higher order and bear on no problem page. Rohrbach's constant c2=1c_2=1, the trivial n2(k)≥(k/2)2+O(k)n_2(k)\ge(k/2)^2+O(k), is recorded on p. 118 as the previous record. The problem page reads (3) on the page images at statement depth; the parameter optimization was not reproduced and no proof was checked.

Results.

  • Satz 1 (p. 119; Bemerkung and proof pp. 120--121): from hh sets containing 00 whose union is an interval basis of order hh for nhn_h with one summand from each set, and natural numbers αh+1\alpha_{h+1}, th+1t_{h+1}, i≤hi\le h, it builds an interval basis of order h+1h+1 of the same kind for nh+1=((th+1+1)αh+1+(th+1−1)ji,h)rh+nhn_{h+1}=((t_{h+1}+1)\alpha_{h+1}+(t_{h+1}-1)j_{i,h})r_h+n_h; applied to {0,1,…,α1}\{0,1,\ldots,\alpha_1\} it gives B2B_2 (p. 121), and applied again to B2B_2 with i=2i=2 it gives B3B_3 (p. 122).
  • Satz 2 (p. 123; proof pp. 123--124): for fixed h≥2h\ge2 and k→∞k\to\infty, nh(k)≥(87)h/2(kh)h+O(kh−1)n_h(k)\ge(\frac87)^{h/2}(\frac kh)^h+O(k^{h-1}) for even hh and nh(k)≥3227(87)(h−3)/2(kh)h+O(kh−1)n_h(k)\ge\frac{32}{27}(\frac87)^{(h-3)/2}(\frac kh)^h+O(k^{h-1}) for odd hh; the page also records equation (4), n3(k)≥3227(k3)3+O(k2)n_3(k)\ge\frac{32}{27}(\frac k3)^3+O(k^2) (p. 123).
  • Equation (3) (pp. 118 and 123): n2(k)≥87(k2)2+O(k)n_2(k)\ge\frac87(\frac k2)^2+O(k), from the order-2 basis B2B_2 of p. 121 with t2=3t_2=3 and α1=k/7+O(1)\alpha_1=k/7+O(1); the h=2h=2 case of Satz 2.

No file of this source is held: no license on record permits its redistribution, and the card cites the edition it names above.