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受扰球体的静态平衡:单谐类映射、奇偶性障碍与单单静态 regime 的已验证计数反例

Static Equilibria of Perturbed Spheres: A Single-Harmonic Class Map, a Parity Obstruction, and a Certified Counter for the Mono-Monostatic Regime

Vincent Wesley Couey

arXiv 2608.11213首次发表:更新:

AI 中文总结

该研究构造性证明单球谐扰动球体的平衡数公式,揭示单谐无法实现单单静态,提出多谐 regime 的已验证平衡计数方法,解决相关歧义问题。

AI 中文摘要

Varkonyi 和 Domokos 证明,存在齐次凸体,其稳定静态平衡数 S≥1 和不稳定静态平衡数 U≥1 可任意指定,其中 S=U=1 的情况为单单静态 Gomboc。他们的结果是一个存在性命题。我们对最简单的非退化形状给出完整构造性解答:边界为单位球面、经单个实球谐函数 Y_ℓ^m(ℓ≥2,1≤m≤ℓ)径向扰动的齐次体,在 m≥2 时的凸振幅范围内,以及 m=1 时的小振幅范围内,恰好具有 S = U = m(ℓ−m+1) 个稳定和不稳定平衡。对于 m≥2,向谐函数临界点的约化是恒等映射:单个田谐函数的对称性将质心精确固定在原点,因此质心到表面的距离是谐函数的严格递增函数。我们计数 Y_ℓ^m 的临界点,并以指数形式验证 Poincaré-Hopf 平衡,极猴鞍点保持不分裂,指数为 1−m。由此得出三个结论:单个谐函数仅填充 S=U 的对角线,因此次数≥2 的谐函数均非单单静态;任何中心对称(偶次)扰动的 S、U 均为偶数,存在奇偶性障碍;因此单单静态性本质上是多谐的。对八个物体的“先预测后验证”研究与公式完全匹配。对于单单静态体所在的多谐 regime,我们给出一个已验证的平衡计数反例(基于质心到表面距离的区间算术、Krawczyk 唯一性、区间 Hessian 分类、极射赤平极图),给定质心后,可保证既不遗漏也不多计。它验证了特定近球体为单单静态,包括已知的解析参数化,通过已验证计算解决了 drainage-basin 法和基于种子的方法无法明确的问题。

英文摘要

Varkonyi and Domokos proved that homogeneous convex bodies exist with any prescribed numbers $S\ge1$ of stable and $U\ge1$ of unstable static equilibria, the case $S=U=1$ being the mono-monostatic Gomboc. Their result is an existence statement. We give a complete constructive answer for the simplest nondegenerate shapes: a homogeneous body whose boundary is the unit sphere perturbed radially by a single real spherical harmonic $Y_\ell^m$ ($\ell\ge2$, $1\le m\le\ell$) has exactly $S = U = m(\ell-m+1)$ stable and unstable equilibria, for every amplitude in the convex range when $m\ge2$ and for small amplitude when $m=1$. For $m\ge2$ the reduction to the critical points of the harmonic is an identity: the symmetry of a single tesseral harmonic pins the centroid at the origin exactly, so the centroid-to-surface distance is a strictly increasing function of the harmonic. We count the critical points of $Y_\ell^m$ and verify the Poincare-Hopf balance in index form, the polar monkey-saddles persisting unsplit with index $1-m$. Three consequences follow: a single harmonic populates only the diagonal $S=U$, so none of degree $\ge2$ is mono-monostatic; any centrally symmetric (even-degree) perturbation has even $S,U$, a parity obstruction; hence mono-monostaticity is intrinsically multi-harmonic. A predict-then-confirm study on eight bodies matches the formula exactly. For the multi-harmonic regime, where mono-monostatic bodies live, we give a certified equilibrium counter (interval arithmetic on the centroid-to-surface distance, Krawczyk uniqueness, interval-Hessian classification, stereographic polar charts) that, given the centroid, provably neither under- nor over-counts. It certifies specific near-spherical bodies mono-monostatic, including a known analytic parameterization, settling by certified computation a question that drainage-basin and seed-based methods leave ambiguous.

Comments10 pages, 1 figure

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