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 $\mathbb{H}^d$
$\mathbb{H}^d$Published online by Cambridge University Press: 10 March 2023
Consider Bernoulli bond percolation on a graph nicely embedded in hyperbolic space  $\mathbb{H}^d$ in such a way that it admits a transitive action by isometries of
$\mathbb{H}^d$ in such a way that it admits a transitive action by isometries of  $\mathbb{H}^d$. Let
$\mathbb{H}^d$. Let  $p_{\text{a}}$ be the supremum of all percolation parameters such that no point at infinity of
$p_{\text{a}}$ be the supremum of all percolation parameters such that no point at infinity of  $\mathbb{H}^d$ lies in the boundary of the cluster of a fixed vertex with positive probability. Then for any parameter
$\mathbb{H}^d$ lies in the boundary of the cluster of a fixed vertex with positive probability. Then for any parameter  $p < p_{\text{a}}$, almost surely every percolation cluster is thin-ended, i.e. has only one-point boundaries of ends.
$p < p_{\text{a}}$, almost surely every percolation cluster is thin-ended, i.e. has only one-point boundaries of ends.
 $\textbf Z^d$
, many questions and a few answers. Electron. Commun. Prob. 1, 71–82.CrossRefGoogle Scholar
$\textbf Z^d$
, many questions and a few answers. Electron. Commun. Prob. 1, 71–82.CrossRefGoogle Scholar $\mathbb{H}^3$
. Preprint. Available at http://arxiv.org/abs/1303.5624.Google Scholar
$\mathbb{H}^3$
. Preprint. Available at http://arxiv.org/abs/1303.5624.Google Scholar $\infty+1$
 dimensions. In Disorder in Physical Systems, Oxford University Press, New York, pp. 167–190.Google Scholar
$\infty+1$
 dimensions. In Disorder in Physical Systems, Oxford University Press, New York, pp. 167–190.Google Scholar