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PreprintCC BY 4.0arXiv

Funk Beta Balls: Exact Potentials and a Three-Phase Pyramid Diagram

Abstract

In a high-dimensional Funk ball, the endpoint potential makes the forward and reverse distances behave differently, while symmetrization erases the distinction that survives in pyramid limits. For Euclidean beta-type radial measures, we determine the natural-scale limits in all three parameter phases. The divergent phase yields directed Gaussian pyramids indexed by the balance between dimension and radial concentration. A positive limiting parameter yields a Gaussian--chi Funk horocone pyramid, built from Gaussian bases, chi-distributed heights, and a directed endpoint-potential increment, while a vanishing parameter yields the universal directed star pyramid. In the last phase, the dimension-dependent logarithmic contributions cancel exactly, so the conclusion requires no further rate condition.

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BibTeX
@misc{yokota2026funk,
  title = {{Funk Beta Balls: Exact Potentials and a Three-Phase Pyramid Diagram}},
  author = {Shigeaki Yokota},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.27752},
  eprint = {2609.27752},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.27752},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Funk Beta Balls: Exact Potentials and a Three-Phase Pyramid Diagram
AU  - Shigeaki Yokota
PY  - 2026
DA  - 2026/09/01
PB  - arXiv
DO  - 10.48550/arxiv.2609.27752
UR  - https://arxiv.org/abs/2609.27752
AB  - In a high-dimensional Funk ball, the endpoint potential makes the forward and reverse distances behave differently, while symmetrization erases the distinction that survives in pyramid limits. For Euclidean beta-type radial measures, we determine the natural-scale limits in all three parameter phases. The divergent phase yields directed Gaussian pyramids indexed by the balance between dimension and radial concentration. A positive limiting parameter yields a Gaussian--chi Funk horocone pyramid, built from Gaussian bases, chi-distributed heights, and a directed endpoint-potential increment, while a vanishing parameter yields the universal directed star pyramid. In the last phase, the dimension-dependent logarithmic contributions cancel exactly, so the conclusion requires no further rate condition.
ER  -