2016
DOI: 10.1017/s0963548315000401
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Inapproximability of the Partition Function for the Antiferromagnetic Ising and Hard-Core Models

Abstract: Recent inapproximability results of Sly (2010), together with an approximation algorithm presented by Weitz (2006) establish a beautiful picture for the computational complexity of approximating the partition function of the hard-core model. Let λc(T∆) denote the critical activity for the hard-model on the infinite ∆-regular tree. Weitz presented an FPTAS for the partition function when λ < λc(T∆) for graphs with constant maximum degree ∆. In contrast, Sly showed that for all ∆ ≥ 3, there exists ε∆ > 0 such th… Show more

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Cited by 109 publications
(135 citation statements)
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“…On the other side, Sly [Sly10] proved that, unless NP=RP, it is NP-hard to obtain an FPRAS for Δ-regular graphs in the tree nonuniqueness region (i.e., when λ > λc(Δ)). These results were extended to all 2-spin antiferromagnetic models, for the positive side see [SST12,LLY13] and for the negative side see [SS12,GSV12]. For 2-spin antiferromagnetic models, this establishes a beautiful picture connecting the computational complexity of approximating the partition function to statistical physics phase transitions in the infinite tree.…”
Section: Introductionmentioning
confidence: 71%
“…On the other side, Sly [Sly10] proved that, unless NP=RP, it is NP-hard to obtain an FPRAS for Δ-regular graphs in the tree nonuniqueness region (i.e., when λ > λc(Δ)). These results were extended to all 2-spin antiferromagnetic models, for the positive side see [SST12,LLY13] and for the negative side see [SS12,GSV12]. For 2-spin antiferromagnetic models, this establishes a beautiful picture connecting the computational complexity of approximating the partition function to statistical physics phase transitions in the infinite tree.…”
Section: Introductionmentioning
confidence: 71%
“…We will prove here that the convergence of BP provides the existence of a distance function Φ satisfying (7). We defer the technical proof of (6) to Section A of the appendix.…”
Section: Path Coupling Distance Functionmentioning
confidence: 94%
“…On the other side, Sly [33] (extended in [6,7,34,8]) has established that, unless N P = RP , for all ∆ ≥ 3, there exists γ > 0, for all λ > λ c (∆), there is no polynomial-time algorithm for triangle-free ∆-regular graphs to approximate the partition function within a factor 2 γn .…”
Section: Introduction Backgroundmentioning
confidence: 99%
“…For general graphical models, if only knowing the parameters B e 's and d, one cannot expect much improvement over this sufficient condition. For example, for the Ising model (ferromagnetic or anti-ferromagnetic, with arbitrary local fields) on graphs with maximum degree ∆ with inverse temperature β, the bound (4) translates to a condition B e = e −2|β| > 1 − 1 4∆ + o( 1 ∆ ); while the sampling problem (even in a static and approximate setting) for the anti-ferromagnetic Ising model in the "non-uniqueness regime", where e −2|β| < 1 − 2 ∆ , is NP-hard [13]. While this sufficient condition on general graphical models focuses on graphical models with soft constraints, our dynamic sampling algorithm is not restricted to such settings.…”
Section: The Running Time Of the Algorithmmentioning
confidence: 99%
“…This bound is asymptotically tight. In the "non-uniqueness regime" where e −2|β| < 1 − 2 ∆ , for the anti-ferromagnetic Ising model, even static and approximate sampling is intractable [13]; and for the ferromagnetic Ising model, by an argument as in [7] there cannot exist such local and parallel sampling algorithms (even for static and approximate sampling) due to the reconstructibility of the ferromagnetic Ising model in the non-uniqueness regime on locally tree-like graphs [3,14].…”
Section: Dynamic Sampling From the Spin Systemsmentioning
confidence: 99%