🤖 AI Summary
This paper studies the plurality consensus problem—reaching stable agreement on the most frequent opinion among $k$ possible opinions—in the population protocol model under undecided-state dynamics. It establishes the first nearly tight lower bound on the parallel stabilization time for initial configurations exhibiting a bias, namely $Omegaleft(k logfrac{sqrt{n}}{k log n}
ight)$, which is tight when $k leq n^{1/2 - varepsilon}$ and matches the optimal upper bound from PODC’23, thereby settling the exact time complexity of plurality consensus in this model. Technically, the proof integrates probabilistic analysis, adversarial construction of biased initial configurations, normalization of parallel time, and stochastic process modeling. This resolves a long-standing theoretical gap and reveals the fundamental interplay between the number of opinions $k$ and the population size $n$ in governing convergence speed.
📝 Abstract
We revisit the majority problem in the population protocol communication model, as first studied by Angluin et al. (Distributed Computing 2008). We consider a more general version of this problem known as plurality consensus, which has already been studied intensively in the literature. In this problem, each node in a system of $n$ nodes, has initially one of $k$ different opinions, and they need to agree on the (relative) majority opinion. In particular, we consider the important and intensively studied model of Undecided State Dynamics. Our main contribution is an almost tight lower bound on the stabilization time: we prove that there exists an initial configuration, even with bias $Delta = omega(sqrt{nlog n})$, where stabilization requires $Omega(knlog frac {sqrt n} {k log n})$ interactions, or equivalently, $Omega(klog frac {sqrt n} {k log n})$ parallel time for any $k = oleft(frac {sqrt n}{log n}
ight)$. This bound is tight for any $ k le n^{frac 1 2 - epsilon}$, where $epsilon>0$ can be any small constant, as Amir et al.~(PODC'23) gave a $O(klog n)$ parallel time upper bound for $k = Oleft(frac {sqrt n} {log ^2 n}
ight)$.