2015
DOI: 10.1080/15326349.2015.1018441
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Slow Transitions and Starvation in Dense Random-Access Networks

Abstract: 2 We consider dense wireless random-access networks, modeled as systems of particles with hardcore interaction. The particles represent the network users that try to become active after an exponential back-off time, and stay active for an exponential transmission time. Due to wireless interference, active users prevent other nearby users from simultaneous activity, which we describe as hardcore interaction on a conflict graph. We show that dense networks with aggressive back-off schemes lead to extremely slow … Show more

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Cited by 3 publications
(3 citation statements)
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“…We briefly outline here the proof strategy of Theorem , to which is devoted the rest of this section. As illustrated by the state space diagram in Figure , there is not a unique bottleneck separating the stable configurations (this was the case for complete partite graphs ) and there are in fact exponentially many possible ways for the Markov chain false{Xtβfalse}tdouble-struckN to make such transitions. This makes the task of identifying the energy barrier between stable configurations much harder.…”
Section: Energy Landscape Analysismentioning
confidence: 99%
See 1 more Smart Citation
“…We briefly outline here the proof strategy of Theorem , to which is devoted the rest of this section. As illustrated by the state space diagram in Figure , there is not a unique bottleneck separating the stable configurations (this was the case for complete partite graphs ) and there are in fact exponentially many possible ways for the Markov chain false{Xtβfalse}tdouble-struckN to make such transitions. This makes the task of identifying the energy barrier between stable configurations much harder.…”
Section: Energy Landscape Analysismentioning
confidence: 99%
“…Tunneling phenomena of the hard-core model have already been studied on complete partite graphs [26,27] and on square grid graphs [20]. In this work we focus on the case where Λ is a finite triangular lattice.…”
Section: Introductionmentioning
confidence: 99%
“…In order to bound the mixing time of the activity process {X C (t)} t≥0 , we will make use of the continuous-time counterpart of that theorem, which is summarized in the following lemma, see [19,Lemma 7.1] for a proof. Lemma 6.2.…”
Section: Asymptotic Lower Bound For the Mixing Timementioning
confidence: 99%