Time vs. Information Tradeoffs for Leader Election in Anonymous Trees
May 16, 2015 Β· Declared Dead Β· π ACM-SIAM Symposium on Discrete Algorithms
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Authors
Christian Glacet, Avery Miller, Andrzej Pelc
arXiv ID
1505.04308
Category
cs.DC: Distributed Computing
Cross-listed
cs.DS
Citations
39
Venue
ACM-SIAM Symposium on Discrete Algorithms
Last Checked
3 months ago
Abstract
The leader election task calls for all nodes of a network to agree on a single node. If the nodes of the network are anonymous, the task of leader election is formulated as follows: every node $v$ of the network must output a simple path, coded as a sequence of port numbers, such that all these paths end at a common node, the leader. In this paper, we study deterministic leader election in anonymous trees. Our aim is to establish tradeoffs between the allocated time $Ο$ and the amount of information that has to be given $\textit{a priori}$ to the nodes to enable leader election in time $Ο$ in all trees for which leader election in this time is at all possible. Following the framework of $\textit{algorithms with advice}$, this information (a single binary string) is provided to all nodes at the start by an oracle knowing the entire tree. The length of this string is called the $\textit{size of advice}$. For an allocated time $Ο$, we give upper and lower bounds on the minimum size of advice sufficient to perform leader election in time $Ο$. We consider $n$-node trees of diameter $diam \leq D$. While leader election in time $diam$ can be performed without any advice, for time $diam-1$ we give tight upper and lower bounds of $Ξ(\log D)$. For time $diam-2$ we give tight upper and lower bounds of $Ξ(\log D)$ for even values of $diam$, and tight upper and lower bounds of $Ξ(\log n)$ for odd values of $diam$. For the time interval $[Ξ²\cdot diam, diam-3]$ for constant $Ξ²>1/2$, we prove an upper bound of $O(\frac{n\log n}{D})$ and a lower bound of $Ξ©(\frac{n}{D})$, the latter being valid whenever $diam$ is odd or when the time is at most $diam-4$. Finally, for time $Ξ±\cdot diam$ for any constant $Ξ±<1/2$ (except for the case of very small diameters), we give tight upper and lower bounds of $Ξ(n)$.
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