Finite-Defect Rigidity and the Minimum Spherical 4-Design on the Two-Sphere
Abstract
We prove that every equal-weight spherical $4$-design on ๐2 has at least twelve points. Since the regular icosahedron is a spherical $5$-design, this determines the exact minimumN4(๐2)=12;equivalently, no such design has $9$, $10$ or $11$ points.The proof is part of a finite-defect theory. If a spherical 2m-design has corank c=Nโdim Pm, its Naimark complement consists of unit vectors uxโ๐cโ1 forming a spherical $2$-design and satisfying the exact couplinguxยท uy=โ(Km(d)(xยท y))/c (xโ y).This gives a pairwise kernel bound, an antipodal lower bound, Cayley-Bacharach information, and uniform lower bounds for multiplicative-relation spaces. In corank one the design splits into two equal spherical m-designs. We derive a residue formula for its signed Schoenberg coefficients; the coefficient of degree m+3 is negative exactly when 3โค dโค m+1, excluding corank one throughout that range. At strengths four and six the only examples in any dimension are the regular hexagon and octagon, respectively.In corank two the complement is a circle Gale frame. Multiplication by its phase forces at least dโ1 linear-quadratic aliases and yields exact norm and socle identities in every dimension. For eleven nodes on ๐2, two aliases produce a real harmonic cubic and a Hermitian quartic matrix. A matrix-valued Cayley-Bacharach argument eliminates the generic branch; the exceptional branch reduces to a Pauli normal form and contradicts the second moments. In dimensions dโฅ4 the corank-two problem remains open; we identify a forced quadratic socle as the obstruction to extending the present argument.
Related
- Minimum energy paths for defect annihilation in finite dodecagonal quasicrystal clusters
- Quadratic-Defect Completions of Spherical $2$-Design Orbits
- Scalar curvature rigidity of small spherical caps with arbitrary fill-ins
- Smallest quotients and profinite rigidity of irreducible spherical type Artin groups
- Sharp local scalar-curvature rigidity of spherical caps
BibTeX
@misc{singh2026finitedefect,
title = {{Finite-Defect Rigidity and the Minimum Spherical 4-Design on the Two-Sphere}},
author = {Shalender Singh and Vishnupriya Singh},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.31689},
eprint = {2609.31689},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.31689},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Finite-Defect Rigidity and the Minimum Spherical 4-Design on the Two-Sphere
AU - Shalender Singh
AU - Vishnupriya Singh
PY - 2026
DA - 2026/09/16
PB - arXiv
DO - 10.48550/arxiv.2609.31689
UR - https://arxiv.org/abs/2609.31689
AB - We prove that every equal-weight spherical $4$-design on ๐^2 has at least twelve points. Since the regular icosahedron is a spherical $5$-design, this determines the exact minimumN_4(๐^2)=12;equivalently, no such design has $9$, $10$ or $11$ points.The proof is part of a finite-defect theory. If a spherical 2m-design has corank c=Nโdim P_m, its Naimark complement consists of unit vectors u_xโ๐^cโ1 forming a spherical $2$-design and satisfying the exact couplingu_xยท u_y=โ(K_m^(d)(xยท y))/c (xโ y).This gives a pairwise kernel bound, an antipodal lower bound, Cayley-Bacharach information, and uniform lower bounds for multiplicative-relation spaces. In corank one the design splits into two equal spherical m-designs. We derive a residue formula for its signed Schoenberg coefficients; the coefficient of degree m+3 is negative exactly when 3โค dโค m+1, excluding corank one throughout that range. At strengths four and six the only examples in any dimension are the regular hexagon and octagon, respectively.In corank two the complement is a circle Gale frame. Multiplication by its phase forces at least dโ1 linear-quadratic aliases and yields exact norm and socle identities in every dimension. For eleven nodes on ๐^2, two aliases produce a real harmonic cubic and a Hermitian quartic matrix. A matrix-valued Cayley-Bacharach argument eliminates the generic branch; the exceptional branch reduces to a Pauli normal form and contradicts the second moments. In dimensions dโฅ4 the corank-two problem remains open; we identify a forced quadratic socle as the obstruction to extending the present argument.
ER -