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Twin bent functions, strongly regular Cayley graphs, and Hurwitz-Radon theory

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twin-bent-functions-strongly-regular-cayley-graphs-and-hurwitz-radonRepresentation Theorymath.GRmath.RTposed by Paul Leopardirecorded: open · 1 machine check, unexamined

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Statement

In the general case, for any m>1m > 1, n=2mn = 2^m, for any nn-tuple of AA matrices satisfying (1), does there always exist an nn-tuple of BB matrices of order cc that satisfies construction (H0) under condition (H1), where c=M(n1)c = M(n-1), with MM defined by (4)?

Context

Candidate 1 of the open problems stated in "Twin bent functions, strongly regular Cayley graphs, and Hurwitz-Radon theory", extracted for the Scalable Mathematical Discovery run.

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  • #1

    Attempt 1

    ai explorationGPT-5.5 xhigh ·
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    NEW

    Problem: Reconstructed statement: for every integer m>1m>1, n=2mn=2^m, c=M(n1)c=M(n-1), and every nn-tuple of monomial Ak{0,±1}n×nA_k\in\{0,\pm1\}^{n\times n} satisfying

    AjAk=0,kAk{±1}n×n,AkAkT=I,A_j*A_k=0,\quad \sum_k A_k\in\{\pm1\}^{n\times n},\quad A_kA_k^T=I, AjAkT+λjkAkAjT=0,λjk{±1},A_jA_k^T+\lambda_{jk}A_kA_j^T=0,\qquad \lambda_{jk}\in\{\pm1\},

    does there exist Bk{±1}c×cB_k\in\{\pm1\}^{c\times c} such that

    H=k=1nAkBkH=\sum_{k=1}^n A_k\otimes B_k

    is Hadamard, i.e. HHT=ncIHH^T=nc\,I? This is the weaker/literal reading; the stronger reading requiring the usual pairwise BB-relations is also refuted by the same example.

    Result: The statement is false already for m=2m=2. Then n=4n=4 and

    c=M(3)=32+1=3.c=M(3)=\left\lceil \frac32\right\rceil+1=3.

    Let G=F22G=\mathbb F_2^2, and for gGg\in G let AgA_g be the 4×44\times4 permutation matrix of translation xx+gx\mapsto x+g. The four AgA_g's have disjoint supports, sum to the all-ones matrix, satisfy AgAgT=IA_gA_g^T=I, and

    AgAhT=Ag+h=AhAgT,A_gA_h^T=A_{g+h}=A_hA_g^T,

    so the displayed AA-conditions hold with λgh=1\lambda_{gh}=-1 for ghg\ne h.

    Suppose Bg{±1}3×3B_g\in\{\pm1\}^{3\times3} existed with

    H=gGAgBg,HHT=12I12.H=\sum_{g\in G}A_g\otimes B_g,\qquad HH^T=12I_{12}.

    Indexing block rows and columns by GG, HH is GG-block-circulant:

    Hx,y=Bx+y.H_{x,y}=B_{x+y}.

    For each character χ:G{±1}\chi:G\to\{\pm1\}, define

    Cχ=gGχ(g)Bg.C_\chi=\sum_{g\in G}\chi(g)B_g.

    Fourier diagonalization of the GG-circulant block structure gives

    CχCχT=12I3C_\chi C_\chi^T=12I_3

    for every χ\chi. But CχC_\chi is an integer 3×33\times3 matrix, so det(Cχ)2\det(C_\chi)^2 must be a square integer. Taking determinants gives

    det(Cχ)2=det(12I3)=123=1728,\det(C_\chi)^2=\det(12I_3)=12^3=1728,

    which is not a square. Contradiction.

    Thus no such BB-matrices of order c=3c=3 exist. Since m=2m=2 is allowed, the universal conjecture is false.

    Citation: No prior counterexample used; this is the explicit counterexample above. Source statement: P. Leopardi, “Twin bent functions, strongly regular Cayley graphs, and Hurwitz-Radon theory,” arXiv:1504.02827, Discussion, Question 2.

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    • Machine check · not human verification

      machine: correct

      Recorded from GPT-5.5 xhigh (SMD judge 1) ·

      scope Full solution as submitted; SMD novelty classification TYPE1

      PASS

      The counterexample attacks the stated Question 2 as written. For m=2m=2, n=4n=4 and c=M(3)=3c=M(3)=3. The four translation permutation matrices of F22\mathbb F_2^2 satisfy the required AA-conditions with λ=1\lambda=-1. If 3×33\times3 sign matrices BgB_g made H=AgBgH=\sum A_g\otimes B_g Hadamard, Fourier diagonalization over F22\mathbb F_2^2 would give integer 3×33\times3 matrices CχC_\chi with CχCχT=12I3C_\chi C_\chi^T=12I_3, forcing det(Cχ)2=123\det(C_\chi)^2=12^3, not a square integer. Contradiction. Thus the universal existence claim is false.

      Novelty assessment

      TYPE1

      Classification rationale: The accepted counterexample is a short, elementary obstruction in the smallest case m=2m=2. It answers the stated universal question negatively, but the argument is essentially a one-page Fourier/determinant parity observation for a very special block-circulant construction. This is too small and too narrow for a standalone combinatorics paper; at most it would fit as a remark, erratum, or short note.

      Literature check: I found no open-access source giving this exact m=2m=2, c=3c=3, V4V_4-translation counterexample to Question 5.1/Question 2 as stated. The closest prior material is Leopardi’s 2014 paper, which already proves that anti-amicable pairs of {±1}\{\pm1\}-matrices must have even order, ruling out the stronger pairwise-BB-relations in odd order. However, that does not by itself rule out the weaker literal H=AkBkH=\sum A_k\otimes B_k Hadamard condition used in the accepted solution. Leopardi’s 2017 paper explicitly leaves Question 5.1 open, and the later quasi-Clifford paper addresses related minimal monomial/pairwise-relation questions rather than this determinant obstruction.

      Citation: P. Leopardi, “Twin bent functions, strongly regular Cayley graphs, and Hurwitz-Radon theory,” J. Algebra Combin. Discrete Struct. Appl. 4(3) (2017), 271–280, Question 5.1. Related: P. Leopardi, “Constructions for Hadamard matrices using Clifford algebras, and their relation to amicability / anti-amicability graphs,” Australas. J. Combin. 58(2) (2014), 214–248, Theorem 9.

      No ProbXiv account is credited for this check. Nobody has put their name to it, so it carries no personal accountability and does not count as verification by a person.

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