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Spherical Designs with Infinite Harmonic Strength

Published 2 Jul 2026 in math.CO | (2607.01761v1)

Abstract: In this paper, we study the existence problem for spherical (T)-designs on the (d)-dimensional sphere, where (T) is an infinite subset of (\mathbb N). We show that, if (d\ge 2), then a finite subset of (Sd) has infinite harmonic strength if and only if it is antipodal. For (d=1), we show that infinite strength spherical designs are exactly cyclotomic designs, and we characterize their existence in terms of certain (0)-(1) polynomials. We also prove that the harmonic strength of every infinite strength spherical design has the weak GCD property. Finally, for a given infinite subset (T\subset \mathbb N) with the weak GCD property, we give a finite procedure to decide whether there exists (X\subset S1) such that (\operatorname{Hst}(X)=T), and apply this criterion to concrete existence and non-existence examples.

Summary

  • The paper establishes that for dimensions d ≥ 2, a finite design has infinite harmonic strength if and only if it is antipodal.
  • It characterizes S¹ designs by proving that only cyclotomic designs achieve infinite harmonic strength through a rich periodic structure.
  • Using algebraic techniques and polynomial criteria, the work provides explicit decidability conditions and bounds linking harmonic strength with combinatorial properties.

Spherical Designs with Infinite Harmonic Strength

Introduction and Framework

The study of spherical designs—finite subsets of the dd-dimensional sphere SdS^d whose pointwise averages match exact spherical averages for classes of polynomials—sits at the intersection of combinatorics, harmonic analysis, and algebraic geometry. For a non-empty finite set XSd,X\subset S^d, the traditional notion of a spherical tt-design requires that 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi) hold exactly for all polynomials ff of degree at most tt. Extending this, the concept of spherical TT-designs considers arbitrary (possibly infinite) sets of polynomial degrees TNT\subset\mathbb{N}, leading to the central notion of harmonic strength: $\operatorname{Hst}(X) = \left\{ k\in\mathbb{N} : \sum_{\xi\in X} P(\xi) = 0 \text{ for all } P\in\Harm_k(d+1)\right\}$ where SdS^d0 is the space of degree-SdS^d1 homogeneous harmonic polynomials in SdS^d2 variables.

The paper investigates the existence and classification of finite SdS^d3 with infinite SdS^d4 (termed infinite strength spherical designs), providing a sharp dichotomy based on the dimension SdS^d5 and uncovering strong algebraic constraints on the possible SdS^d6 for which such SdS^d7 can exist.

Classification of Infinite Strength Spherical Designs

Higher Dimensions: SdS^d8

For SdS^d9, the main result is a complete classification:

Theorem: A finite subset XSd,X\subset S^d,0 is an infinite strength spherical design if and only if XSd,X\subset S^d,1 is antipodal (i.e., XSd,X\subset S^d,2).

The proof leverages inequalities for Jacobi (specifically, Gegenbauer) polynomials [HS2014] applied to the duality of harmonic polynomials and pointwise structure on the sphere. Using these inequalities, the authors show that for non-antipodal XSd,X\subset S^d,3 and XSd,X\subset S^d,4, the harmonic strength can only contain finitely many indices—eventually, the moment sum condition fails except possibly for odd degrees if and only if XSd,X\subset S^d,5 maintains antipodal symmetry.

Moreover, the paper gives explicit (dimension and set-dependent) upper bounds on the maximal degree occurring in the harmonic strength, indicating, for arbitrary finite XSd,X\subset S^d,6 in XSd,X\subset S^d,7 with XSd,X\subset S^d,8, that only for small XSd,X\subset S^d,9 can tt0 hold unless antipodality is present.

If tt1 is antipodal, then all odd tt2 belong to tt3, and the even part is finite and explicitly bounded.

Dimension tt4: Cyclotomic Designs

In the case tt5, the landscape changes dramatically. The unit circle admits much richer combinatorial structures. Here the following classification is established:

Theorem: For tt6, tt7 has infinite harmonic strength if and only if tt8 is a cyclotomic design.

Cyclotomic designs generalize both antipodal and group-type designs. The paper provides an algebraic characterization for tt9: 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)0 is a cyclotomic design if its points can be partitioned into nontrivial sets each forming a regular polygon (possibly with distinct periods) modulated by a group of roots of unity.

Using complex moments—a scalar representation via 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)1—and leveraging the Skolem–Mahler–Lech theorem [Lech, Skolem] on the zeros of recurrence sequences, the authors show that 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)2 with infinite support must exhibit a periodic structure, corresponding precisely to the combinatorics of cyclotomic partitions.

Harmonic Strength and the Weak GCD Property

A central algebraic result is that the infinite subsets 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)3 which occur as harmonic strengths of finite designs must possess the weak GCD property: there exist finite 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)4, period 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)5, and 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)6 such that

1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)7

For 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)8, any antipodal 1SdSdf(ξ)dξ=1XξXf(ξ)\frac{1}{|S^d|}\int_{S^d} f(\xi)d\xi = \frac{1}{|X|}\sum_{\xi\in X} f(\xi)9 realizes only ff0 with ff1 (i.e., odd ff2 plus a finite set), while for ff3, cyclotomic designs realize those ff4 with arbitrarily large periods, but no further.

A highly nontrivial aspect is proving that ff5 for any infinite strength design must be periodic in this strong sense; the proof relies on transcendence results (Baker's theorem [B1975]) and careful analysis of the algebraic representation of ff6 via polynomials.

Decidability: Existence for a Given ff7

The inverse problem—given ff8 with the weak GCD property, does some ff9 exist with tt0?—is resolved constructively.

Theorem: Such tt1 exists if and only if there exists a finite collection of nonzero tt2-tt3 polynomials tt4 of degree tt5 such that

tt6

where tt7 is the tt8-th cyclotomic polynomial.

This algebraic criterion provides a reduction to finite computation (as there are finitely many tt9-TT0 polynomials of degree TT1), making the existence of infinite strength designs fully decidable for any candidate TT2. The paper demonstrates both explicit constructions (e.g., for all TT3 corresponding to TT4) and nonexistence, such as for TT5 missing all indices with certain residues modulo TT6.

Bounds and Fisher-Type Inequalities

The paper compares its results with Fisher-type lower bounds on spherical designs [D1977]. For TT7, the size of TT8 with prescribed harmonic strength must grow at least polynomially in the degree, even for single TT9, with bounds depending on the maximal inner product among points. These are sharp in various regimes and demonstrate that antipodal or cyclotomic structure does not lead to "too small" infinite strength sets for high degrees.

Implications and Future Directions

The results have deep implications for both the combinatorics of design theory and harmonic analysis. In higher dimensions, infinite strength is sharply limited to antipodal sets, highlighting robust rigidity. For TNT\subset\mathbb{N}0, the picture is richer: the algebraic machinery not only yields classification, but also algorithmic existential answers, and opens connections to the geometry of cyclotomic fields and the algebraic theory of moments.

The algebraic approach, grounded in sophisticated tools such as transcendence theory and recurrence sequence theorems, is striking in its scope and applicability. The methods suggest explicit strategies for constructing or ruling out spherical designs with intricate combinatorial properties, with potential implications for coding theory, numerical integration, and harmonic analysis on other spaces.

Open directions include the quantification and minimization of TNT\subset\mathbb{N}1 for prescribed TNT\subset\mathbb{N}2, further refinement of periodicity constraints, and generalization to more exotic manifolds or spaces with other symmetry groups. Optimization problems regarding the minimal size or configuration for a given harmonic strength are also left as challenging avenues for subsequent work.

Conclusion

This paper delivers a rigorous characterization of infinite strength spherical designs, demonstrating that in all dimensions but one, antipodality is necessary, and for TNT\subset\mathbb{N}3, designs must be cyclotomic. The mapping of harmonic strength to algebraic properties of polynomials and explicit decidability criteria fully resolves the existence question for infinite TNT\subset\mathbb{N}4-designs. The results integrate sharp combinatorial, analytic, and algebraic analysis, offering an authoritative reference for both the theory and constructive aspects of spherical TNT\subset\mathbb{N}5-designs.


References:

  • "Spherical Designs with Infinite Harmonic Strength" (2607.01761)
  • Haagerup & Schlichtkrull, "Inequalities for Jacobi polynomials" [HS2014]
  • Delsarte, Goethals, & Seidel, "Spherical codes and designs"
  • Baker, "Transcendental Number Theory" [B1975]
  • Lech, "A note on recurring series"; Skolem, "Einige Sätze über gewisse Reihenentwicklungen..."

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