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$841$点亲吻排列在${\mathbb R}^{12}$背后的四元数构造

A quaternionic construction behind $841$-point kissing arrangement in ${\mathbb R}^{12}$

Rustem Takhanov

arXiv 2609.09179首次发表:更新:

发表机构

Nazarbayev University(纳扎尔巴耶夫大学)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

本文通过四元数结构解释了$\mathbb R^{12}$中$841$点亲吻排列纪录,构造了$840$点模型并推广到$4k$维。

AI 中文摘要

最近,通过优化(Takhanov-Assylbekov-Yun,2026)在$\mathbb R^{12}$中数值上获得了$841$点的新纪录亲吻排列。该构型以坐标文件形式发布,没有其结构的数学描述。本文的目的是提供这样的描述。关键观察是,一旦我们将$\mathbb R^{12}\cong \mathbb H^3$视为四元数代数的三个副本的笛卡尔积,几何就变得透明。我们首先引入一个新的具有特定四元数结构的$840$点亲吻排列。它由三个相互正交的正则$24$胞腔组成,分别支撑在三个四元数坐标因子$\mathbb H\times\{0\}\times\{0\}$、$\{0\}\times\mathbb H\times\{0\}$、$\{0\}\times\{0\}\times\mathbb H$上,以及两个$384$点族,这些族通过将形如$$\{(u,v,w)\in (\mathbb F_2^2)^3\mid u+v+w=\eta\}$$的仿射集合提升为四元数三元组(其分量属于二元八面体群$2O$),然后应用适当的分量旋转和加权获得。该构造的一个显著特征是三个四元数因子之间存在明显的不对称性。对于移除第三个$24$胞腔后获得的$816$个向量,大部分平方范数集中在前两个四元数坐标中,而第三个坐标系统地承载较少质量。因此,第三个四维因子比前两个包含更多可用空间。然后我们证明这个$840$点构型为数值$841$点纪录提供了自然的结构模型。最后,我们引入在维数可被$4$整除时的一般四元数构造的概念,并检查${\mathbb R}^{4k}$($k\leq 5$)中的纪录亲吻排列是否允许四元数构造。

英文摘要

Recently, a new record kissing arrangement of $841$ points in $\mathbb R^{12}$ was obtained numerically by optimization (Takhanov-Assylbekov-Yun, 2026). The configuration was released as a coordinate file, without a mathematical description of its structure. The purpose of this paper is to provide such a description. The key observation is that the geometry becomes transparent once we regard $\mathbb R^{12}\cong \mathbb H^3$ as the Cartesian product of three copies of the quaternion algebra. We first introduce a new $840$-point kissing arrangement with a certain quaternionic structure. It consists of three mutually orthogonal regular $24$-cells, supported on the three quaternionic coordinate factors $\mathbb H\times\{0\}\times\{0\}$, $\{0\}\times\mathbb H\times\{0\}$, $\{0\}\times\{0\}\times\mathbb H$, together with two $384$-point families obtained by lifting affine sets of the form $$\{(u,v,w)\in (\mathbb F_2^2)^3\mid u+v+w=η\},$$ to quaternionic triples (whose components belong to the binary octahedral group $2O$) and then applying suitable component-wise rotations and weightings. A characteristic feature of this construction is a pronounced asymmetry among the three quaternionic factors. For the $816$ vectors obtained after removing the third $24$-cell, most of the squared norm is concentrated in the first two quaternionic coordinates, while the third coordinate carries systematically less mass. Thus, the third four-dimensional factor contains more available space than the first two. We then show that this $840$-point configuration provides a natural structural model for the numerical $841$-point record. Finally, we introduce a notion of the general quaternionic construction in dimensions divisible by $4$, and check that record kissing arrangements in ${\mathbb R}^{4k}$, $k\leq 5$, admit a quaternionic construction.

论文原文

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