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Asymptotic counting exponent for partial Hadamard matrices (C23cC_{23c})

Asymptotic counting exponent for partial Hadamard matrices: determine C23cC_{23c} or improve its bounds; the repository records 1 (lower) and 3 (upper).

Editorial MSC2020 classification. Original article codes and source evidence are recorded in the literature directory.

Licensed source statementAs of Repository table at commit 2c1968c (2026-09-26); open while the recorded lower and upper bounds differSource & evidence ↓

Problem statement

For integers n≥2n \ge 2 and t≥1t \ge 1, an n×tn \times t partial Hadamard matrix is a matrix with entries in {±1}\{\pm 1\} whose rows are pairwise orthogonal. Let Nn,tN_{n,t} denote the number of such matrices. For every fixed nn one has

Nn,4t=[1+o(1)] An,4tas t→∞,N_{n,4t} = [1+o(1)]\,A_{n,4t} \qquad\text{as } t \to \infty,

where

An,4t:=24nt+(n−1)2(8πt)−n(n−1)/4.A_{n,4t} := 2^{4nt+(n-1)^2}(8\pi t)^{-n(n-1)/4}.

[Davis2026-def-partial] [Davis2026-fixed-n-A]

Historically, de Launey–Levin proved the fixed-nn asymptotic Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t}; Canfield later obtained the uniform regime t/n4→∞t/n^4 \to \infty; and the current best result improves this to t/n3→∞t/n^3 \to \infty and shows that Nn,4t/An,4tN_{n,4t}/A_{n,4t} does not converge to 11 when t=Θn3t=\Theta n^3 with Θ\Theta large fixed. Thus the remaining open problem is to determine the correct asymptotics of Nn,4tN_{n,4t} below the cubic scale. [Davis2026-fixed-n-A] [Can2011] [Davis2026-prior-exponents] [Davis2026-change-cubic] [Davis2026-open-below3]

We define C23cC_{23c} to be the smallest admissible exponent α≥1\alpha \ge 1 for which the count Nn,4tN_{n,4t} admits a uniform asymptotic formula throughout the regime t/nα→∞t/n^\alpha \to \infty. The restriction α≥1\alpha \ge 1 is forced by the linear-algebra obstruction 4t≥n4t \ge n. The current best-established range is

1≤C23c≤3.1 \le C_{23c} \le 3.

[DL2010-linear-obstruction] [Davis2026-open-below3] [Davis2026-abstract-cubic]

Lean 4

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Background

  • What is already solved. The narrower problem of determining when the leading term An,4tA_{n,4t} alone is asymptotically correct has exact answer 33. What remains open is whether a corrected asymptotic formula already holds for some exponent below 33. [Davis2026-figure2] [Davis2026-change-cubic]

  • Relation to the Hadamard conjecture. The full Hadamard problem sits at the linear endpoint 4t=n4t=n: the Hadamard conjecture is equivalent to Nn,n>0N_{n,n}>0 whenever nn is divisible by 44. [Davis2026-hadamard-nn]

  • Fixed-nn versus uniform counting. The main difficulty is to keep control when nn grows with tt. [Davis2026-fixed-n-A] [Davis2026-hadamard-nn]

  • Historical formulation of the hard regime. de Launey–Levin already singled out sharper estimates “in the region close to t=nt=n” as an important open problem. [DL2010-near-t=n-open]

References (from the repository page)

  • [Davis2026] Davis, Damek. Counting partial Hadamard matrices in the cubic regime. arXiv:2603.30013 (2026). DOI: 10.48550/arXiv.2603.30013. arXiv PDF: arXiv:2603.30013. Google Scholar
  • [Davis2026-abstract-cubic] loc: arXiv v1 PDF p.1, Abstract. quote: “We give a precise asymptotic formula for the number of n×4tn \times 4t partial Hadamard matrices in the regimes t/n3→∞t/n^3 \to \infty and t/n3→Θt/n^3 \to \Theta for sufficiently large fixed Θ\Theta. This strengthens earlier results of de Launey and Levin, who obtained the asymptotic for t/n12→∞t/n^{12} \to \infty, and of Canfield, who extended this to t/n4→∞t/n^4 \to \infty.”
  • [Davis2026-def-partial] loc: arXiv v1 PDF p.1, Section 1 (Introduction), opening paragraphs. quote: “Rather than constructing full Hadamard matrices, one can study partial ones: an n×tn \times t matrix with entries in {±1}\{\pm1\} is a partial Hadamard matrix if its rows are pairwise orthogonal. Partial Hadamard matrices of width nearly 2n2n are known to exist for large nn by combining constructions from combinatorial design theory [4, 5] with analytic number theory [7] (see [6, Theorem A]). While these results settle existence for widths close to 2n2n, a finer question is to determine how many partial Hadamard matrices there are as a function of nn and tt.”
  • [Davis2026-fixed-n-A] loc: arXiv v1 PDF p.2, Section 1 (Introduction), paragraph preceding Theorem 1.1. quote: “Using this framework, De Launey and Levin [6, Theorem 2] proved that for every fixed n≥2n \ge 2, the number of n×4tn \times 4t partial Hadamard matrices satisfies
Nn,4t=[1+o(1)]An,4t as t→∞,N_{n,4t} = [1 + o(1)] A_{n,4t} \text{ as } t \to \infty,

where An,s:=2ns+2d−n+1(2πs)−d/2A_{n,s} := 2^{ns+2d-n+1}(2\pi s)^{-d/2}.”

  • [Davis2026-hadamard-nn] loc: arXiv v1 PDF p.2, Section 1 (Introduction), paragraph preceding Theorem 1.1. quote: “Since the Hadamard conjecture is equivalent to Nn,n>0N_{n,n} > 0 whenever nn is divisible by 44, one can also ask what happens when nn grows with tt, potentially at a slower rate: does Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t} still hold, and if so, with what corrections?”

  • [Davis2026-prior-exponents] loc: arXiv v1 PDF p.2, Section 1 (Introduction), paragraph preceding Theorem 1.1. quote: “Two prior works address this in the regime t/nα→∞t/n^\alpha \to \infty: (i) De Launey and Levin’s proofs [6, Theorem 4.1] give Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t} as t/n12→∞t/n^{12} \to \infty, though this is never explicitly stated. (ii) Canfield [2] established the same asymptotic as t/n4→∞t/n^4 \to \infty in unpublished work.”

  • [Davis2026-open-below3] loc: arXiv v1 PDF p.2, Section 1 (Introduction), discussion following Theorem 1.1. quote: “Thus the expansion captures the first deviation of Nn,4tN_{n,4t} from the scale An,4tA_{n,4t}. Below α=3\alpha = 3 the asymptotics of Nn,4tN_{n,4t} are open (Figure 2).”

  • [Davis2026-figure2] loc: arXiv v1 PDF p.3, Figure 2 caption. quote: “Each marker indicates the smallest α\alpha for which the corresponding work establishes Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t} as t/nα→∞t/n^\alpha \to \infty. Corollary 4.1 extends this to α=3\alpha = 3. Theorem 1.1 further shows that Nn,4t/An,4tN_{n,4t}/A_{n,4t} has a nonvanishing correction when t/n3t/n^3 converges to a constant.”

  • [Davis2026-change-cubic] loc: arXiv v1 PDF p.22, end of Section 4 (after Corollary 4.1). quote: “Thus Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t} as t/n3→∞t/n^3 \to \infty. Conversely, when t=Θn3t = \Theta n^3 with Θ≥C0\Theta \ge C_0 fixed, the error is O(Θ−2+1/n+e−cn2)O(\Theta^{-2} + 1/n + e^{-cn^2}), so for Θ\Theta large and n→∞n \to \infty the leading correction 1/(48Θ)1/(48\Theta) dominates and Nn,4t/An,4tN_{n,4t}/A_{n,4t} does not converge to 11: the asymptotics of Nn,4tN_{n,4t} change at the cubic scale.”

  • [Can2011] Canfield, E. Rodney. Counting partial Hadamard matrices. Joint Mathematics Meetings (2011), Preliminary report. JMM archive PDF: 1067-05-1695.pdf. Google Scholar

  • [DL2010] de Launey, Warwick; Levin, David A. A Fourier-analytic approach to counting partial Hadamard matrices. Cryptography and Communications 2 (2010), no. 2, 307–334. DOI: 10.1007/s12095-010-0033-z. arXiv PDF: arXiv:1003.4003. Google Scholar

  • [DL2010-linear-obstruction] loc: arXiv v1 PDF p.1, Section 1 (Introduction), definition paragraph. quote: “For non-negative integers nn and tt, a partial Hadamard matrix is an n×tn \times t matrix with ±1\pm1 entries such that the inner product between any two distinct rows equals zero. Note that, since the rows of a partial Hadamard matrix DD form a set of nn independent tt-dimensional real vectors, we must have t≥nt \ge n.”

  • [DL2010-near-t=n-open] loc: arXiv v1 PDF p.4, Section 1 (Introduction), closing paragraph. quote: “While we have left open the important (and probably difficult) problem of obtaining sharper estimates for the integral in equation (3) in the region close to t=nt = n, this paper at the very least introduces an interesting non-symmetric lattice random walk, where an understanding of the early (rather than the asymptotic) behavior of the transition probabilities for the walk is paramount.”

Progress & source assessment

Repository table (commit 2c1968c, 26 September 2026): best known lower bound 1; best known upper bound 3. Values marked with an asterisk have minimal verification.

Known upper bounds

Bound on C23cC_{23c} Reference Comments
1212 [DL2010] Historical first polynomial-range asymptotic-counting bound: the de Launey–Levin argument yields Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t} when t/n12→∞t/n^{12} \to \infty, although that exponent is not isolated as a standalone theorem in the 2010 paper itself. [Davis2026-prior-exponents]
44 [Can2011] Unpublished improvement due to Canfield: Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t} when t/n4→∞t/n^4 \to \infty. [Davis2026-prior-exponents]
33 [Davis2026] Current best upper bound: the cubic-regime result proves Nn,4t∼An,4tN_{n,4t} \sim A_{n,4t} for t/n3→∞t/n^3 \to \infty and shows that a nonvanishing correction survives when t=Θn3t = \Theta n^3 with large fixed Θ\Theta, so the asymptotics change at the cubic scale. [Davis2026-change-cubic] [Davis2026-open-below3]

Known lower bounds

Bound on C23cC_{23c} Reference Comments
11 [DL2010] Admissible exponents cannot be below 11: for any α<1\alpha<1, the regime t/nα→∞t/n^\alpha \to \infty still includes widths with 4t<n4t<n, where an n×4tn \times 4t partial Hadamard matrix cannot exist. [DL2010-linear-obstruction]
References
  1. [1]Davis, Damek; Ivanisvili, Paata; Tao, Terence (maintainers). Optimization Constants in Mathematics, github.com/teorth/optimizationproblems (commit 2c1968c, 26 September 2026). — Asymptotic counting exponent for partial Hadamard matrices ($C_{23c}$) linkApache-2.0 (repository license); constant pages reproduced with attribution; repository references retained.

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