2016
DOI: 10.1090/proc/13311
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Weak Gibbs measures as Gibbs measures for asymptotically additive sequences

Abstract: In this note we prove that every weak Gibbs measure for an asymptotically additive sequences is a Gibbs measure for another asymptotically additive sequence. In particular, a weak Gibbs measure for a continuous potential is a Gibbs measure for an asymptotically additive sequence. This allows, for example, to apply recent results on dimension theory of asymptotically additive sequences to study multifractal analysis for weak Gibbs measure for continuous potentials.

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Cited by 10 publications
(9 citation statements)
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“…, and thus F is asymptotically additive (this was also observed in [33]). However, F admits µ as a Gibbs measure, and also µ as a weak Gibbs measure; in particular, both µ and µ are equilibrium states for F.…”
Section: An Open Question About Almost Additive Sequences and Gibbs M...supporting
confidence: 57%
See 3 more Smart Citations
“…, and thus F is asymptotically additive (this was also observed in [33]). However, F admits µ as a Gibbs measure, and also µ as a weak Gibbs measure; in particular, both µ and µ are equilibrium states for F.…”
Section: An Open Question About Almost Additive Sequences and Gibbs M...supporting
confidence: 57%
“…where C n (x) is the cylinder set of rank n containing x, and we say that µ is a weak Gibbs measure if (3.6) holds with K replaced by K n , where lim n→∞ n −1 log K n = 0. See for example [33].…”
Section: Gibbs and Weak Gibbs Measuresmentioning
confidence: 99%
See 2 more Smart Citations
“…Such sequences of functions are referred to in the literature as almost additive and have been investigated in [4,6,10,21,33]. The condition of almost additivity implies trivially a further property, asymptotic additivity (see for example Feng and Huang [16,Proposition A.5]), which has been applied in [13,16,22]. In another category of works, positivity is replaced by the more general hypothesis of domination: under this hypothesis there exists a continuous splitting R d = U(x) ⊕ V(x), which is preserved by the cocycle, such that A n T (x)u Ce nε A n T (x)v for all unit vectors u ∈ U(x) and v ∈ V(x), for some constants C, ε > 0 (see [7] and references therein).…”
Section: Introductionmentioning
confidence: 99%