A thermodynamical formalism describing mechanical interactions

2014 ◽  
Vol 108 (2) ◽  
pp. 20001 ◽  
Author(s):  
R. F. S. Andrade ◽  
A. M. C. Souza ◽  
E. M. F. Curado ◽  
F. D. Nobre
1994 ◽  
Vol 49 (12) ◽  
pp. 1219-1222 ◽  
Author(s):  
Günter Radons

Abstract Multifractal properties of the invariant densities of correlated random maps are analyzed. It is proven that within the thermodynamical formalism phase transitions for finite correlations may be due to transients. For systems with infinite correlations we show analytically that phase transitions can occur as a consequence of localization-delocalization transitions of relevant eigenfunctions.


2018 ◽  
Vol 20 (10) ◽  
pp. 2357-2412 ◽  
Author(s):  
Paolo Giulietti ◽  
Benoît Kloeckner ◽  
Artur Lopes ◽  
Diego Marcon

1994 ◽  
Vol 49 (12) ◽  
pp. 1235-1237
Author(s):  
Zoltán Toroczkaia ◽  
Áron Péntek

Abstract Here we illustrate the effectiveness of the thermodynamical formalism applied to a well known chaotic phenomenon, the intermittency. This leads us to a new classification for intermittent phe­nomena from the point of view of the generated chaotic phases in the spectrum of the generalized entropies K (q). New types of intermittencies are found related to the absence or presence of phase transitions with infinite jump in K (q). This is underlined with examples. It is also shown via examples that the existence of a marginally stable fixed point in the system is neither necessary nor sufficient for intermittency.


2008 ◽  
Vol 28 (2) ◽  
pp. 501-533 ◽  
Author(s):  
KRERLEY OLIVEIRA ◽  
MARCELO VIANA

AbstractWe develop a Ruelle–Perron–Fröbenius transfer operator approach to the ergodic theory of a large class of non-uniformly expanding transformations on compact manifolds. For Hölder continuous potentials not too far from constant, we prove that the transfer operator has a positive eigenfunction, which is piecewise Hölder continuous, and use this fact to show that there is exactly one equilibrium state. Moreover, the equilibrium state is a non-lacunary Gibbs measure, a non-uniform version of the classical notion of Gibbs measure that we introduce here.


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