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Seeing Through Hyperbolic Space: Visibility for $λ$-Geodesic Hyperplanes

Zakhar Kabluchko, Vanessa Mattutat, Christoph Thaele

Abstract

We study visibility from a fixed point in the presence of a Poisson process of $λ$--geodesic hyperplanes in a $d$-dimensional hyperbolic space. The family of $λ$--geodesic hyperplanes interpolates between totally geodesic hyperplanes and horospheres. Our main result establishes a universality principle for this model: we prove that the fundamental visibility properties are invariant with respect to the parameter $λ\in[0,1]$. Namely, there is a critical intensity $γ_{\mathrm{crit}}>0$ such that the visible region is unbounded with positive probability for $γ< γ_{\mathrm{crit}}$ and almost surely bounded for $γ> γ_{\mathrm{crit}}$. For $d=2$ we establish almost sure boundedness also at criticality. The value for $γ_{\mathrm{crit}}$ is explicit and does not depend on $λ$. In the bounded phase, we show that the mean visible volume is identical with the known formula for $λ=0$. The key integral-geometric step is an explicit computation showing that the measure of $λ$-geodesic hyperplanes hitting a geodesic segment is a linear function of the length of the segment, independent of~$λ$.

Seeing Through Hyperbolic Space: Visibility for $λ$-Geodesic Hyperplanes

Abstract

We study visibility from a fixed point in the presence of a Poisson process of --geodesic hyperplanes in a -dimensional hyperbolic space. The family of --geodesic hyperplanes interpolates between totally geodesic hyperplanes and horospheres. Our main result establishes a universality principle for this model: we prove that the fundamental visibility properties are invariant with respect to the parameter . Namely, there is a critical intensity such that the visible region is unbounded with positive probability for and almost surely bounded for . For we establish almost sure boundedness also at criticality. The value for is explicit and does not depend on . In the bounded phase, we show that the mean visible volume is identical with the known formula for . The key integral-geometric step is an explicit computation showing that the measure of -geodesic hyperplanes hitting a geodesic segment is a linear function of the length of the segment, independent of~.
Paper Structure (14 sections, 13 theorems, 105 equations, 10 figures)

This paper contains 14 sections, 13 theorems, 105 equations, 10 figures.

Key Result

Theorem 1.1

Fix $d\geq 2$, $\gamma>0$ and $0\leq\lambda\leq 1$. Consider the visibility region $Z_{\gamma,\lambda,d}$ of $o$ in a Poisson process of $\lambda$-geodesic hyperplanes in $\mathbb{H}^d$ with intensity measure $\gamma\nu_\lambda^o$.

Figures (10)

  • Figure 1: $\lambda=0, \gamma=2<\gamma_{\mathrm{crit}}$
  • Figure 2: $\lambda=0.5, \gamma=2<\gamma_{\mathrm{crit}}$
  • Figure 3: $\lambda=1, \gamma=2<\gamma_{\mathrm{crit}}$
  • Figure 4: $\lambda=0, \gamma=\pi=\gamma_{\mathrm{crit}}$
  • Figure 5: $\lambda=0.5, \gamma=\pi=\gamma_{\mathrm{crit}}$
  • ...and 5 more figures

Theorems & Definitions (27)

  • Theorem 1.1
  • Lemma 3.1
  • proof
  • Proposition 3.2
  • Lemma 3.3
  • proof
  • Theorem 3.4
  • proof
  • Remark 1
  • Proposition 3.5
  • ...and 17 more