270 research outputs found

    Validity and Failure of the Boltzmann Weight

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    The dynamics and thermostatistics of a classical inertial XY model, characterized by long-range interactions, are investigated on dd-dimensional lattices (d=1,2,d=1,2, and 3), through molecular dynamics. The interactions between rotators decay with the distance rijr_{ij} like~1/rijα1/r_{ij}^{\alpha} (α0\alpha \geq 0), where α\alpha\to\infty and α=0\alpha=0 respectively correspond to the nearest-neighbor and infinite-range interactions. We verify that the momenta probability distributions are Maxwellians in the short-range regime, whereas qq-Gaussians emerge in the long-range regime. Moreover, in this latter regime, the individual energy probability distributions are characterized by long tails, corresponding to qq-exponential functions. The present investigation strongly indicates that, in the long-range regime, central properties fall out of the scope of Boltzmann-Gibbs statistical mechanics, depending on dd and α\alpha through the ratio α/d\alpha/d.Comment: 10 pages, 6 figures. To appear in EP

    Tsallis Distribution Decorated With Log-Periodic Oscillation

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    In many situations, in all branches of physics, one encounters power-like behavior of some variables which are best described by a Tsallis distribution characterized by a nonextensivity parameter qq and scale parameter TT. However, there exist experimental results which can be described only by a Tsallis distributions which are additionally decorated by some log-periodic oscillating factor. We argue that such a factor can originate from allowing for a complex nonextensivity parameter qq. The possible information conveyed by such an approach (like the occurrence of complex heat capacity, the notion of complex probability or complex multiplicative noise) will also be discussed.Comment: 17 pages, 1 figure. The content of this article was presented by Z. Wlodarczyk at the SigmaPhi2014 conference at Rhodes, Greece, 7-11 July 2014. To be published in Entropy (2015

    Some Open Points in Nonextensive Statistical Mechanics

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    We present and discuss a list of some interesting points that are currently open in nonextensive statistical mechanics. Their analytical, numerical, experimental or observational advancement would naturally be very welcome.Comment: 30 pages including 6 figures. Invited paper to appear in the International Journal of Bifurcation and Chao

    Unified model for network dynamics exhibiting nonextensive statistics

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    We introduce a dynamical network model which unifies a number of network families which are individually known to exhibit qq-exponential degree distributions. The present model dynamics incorporates static (non-growing) self-organizing networks, preferentially growing networks, and (preferentially) rewiring networks. Further, it exhibits a natural random graph limit. The proposed model generalizes network dynamics to rewiring and growth modes which depend on internal topology as well as on a metric imposed by the space they are embedded in. In all of the networks emerging from the presented model we find q-exponential degree distributions over a large parameter space. We comment on the parameter dependence of the corresponding entropic index q for the degree distributions, and on the behavior of the clustering coefficients and neighboring connectivity distributions.Comment: 11 pages 8 fig

    Asymptotically scale-invariant occupancy of phase space makes the entropy Sq extensive

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    Phase space can be constructed for NN equal and distinguishable subsystems that could be (probabilistically) either {\it weakly} (or {\it "locally"}) correlated (e.g., independent, i.e., uncorrelated), or {\it strongly} (or {\it globally}) correlated. If they are locally correlated, we expect the Boltzmann-Gibbs entropy SBGkipilnpiS_{BG} \equiv -k \sum_i p_i \ln p_i to be {\it extensive}, i.e., SBG(N)NS_{BG}(N)\propto N for NN \to\infty. In particular, if they are independent, SBGS_{BG} is {\it strictly additive}, i.e., SBG(N)=NSBG(1),NS_{BG}(N)=N S_{BG}(1), \forall N. However, if the subsystems are globally correlated, we expect, for a vast class of systems, the entropy Sqk[1ipiq]/(q1)S_q\equiv k [1- \sum_i p_i^q]/(q-1) (with S1=SBGS_1=S_{BG}) for some special value of q1q\ne1 to be the one which extensive (i.e., Sq(N)NS_q(N)\propto N for NN \to\infty).Comment: 15 pages, including 9 figures and 8 Tables. The new version is considerably enlarged with regard to the previous ones. New examples and new references have been include
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