Issue |
RAIRO-Theor. Inf. Appl.
Volume 49, Number 1, January-March 2015
|
|
---|---|---|
Page(s) | 23 - 45 | |
DOI | https://doi.org/10.1051/ita/2014025 | |
Published online | 23 February 2015 |
Exact location of the phase transition for random (1,2)-QSAT∗,∗∗
1
Aix-Marseille Université, CNRS, LIF UMR 7279,
13288
Marseille,
France
creignou@lif.univ-mrs.fr
2
Aix-Marseille Université, CNRS, I2M UMR 7373,
13453
Marseille,
France
daude@cmi.univ-mrs.fr
3
Institut für Informationsysteme 184/3, Technische Universität
Wien, Favoritenstrasse
9-11
A-1040
Wien,
Austria
uwe@kr.tuwien.ac.at
4
University Grenoble Alpes, IF, 38000
Grenoble,
France
5
CNRS, IF, 38000
Grenoble,
France
raphael.rossignol@ujf-grenoble.fr
Received: 5 May 2014
Accepted: 28 August 2014
The QSAT problem is the quantified version of the SAT problem. We show the existence of a threshold effect for the phase transition associated with the satisfiability of random quantified boolean CNF formulas of the form ∀X∃Yϕ(X,Y), where X has m variables, Y has n variables and each clause in ϕ has one literal from X and two from Y. For such formulas, we show that the threshold phenomenon is controlled by the ratio between the number of clauses and the number n of existential variables. Then we give the exact location of the associated critical ratio c∗: it is a decreasing function of α, where α is the limiting value of m/ log (n) when n tends to infinity. Thus we give a precise location of the phase transition associated with a coNP-complete problem.
Mathematics Subject Classification: 68R01 / 60C05 / 05A16
Key words: Random quantified formulas / satisfiability / phase transition / sharp threshold
© EDP Sciences 2015
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