856 research outputs found

    Lesche Stability of κ\kappa-Entropy

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    The Lesche stability condition for the Shannon entropy [B. Lesche, J. Stat. Phys. 27, 419 (1982)], represents a fundamental test, for its experimental robustness, for systems obeying the Maxwell-Boltzmann statistical mechanics. Of course, this stability condition must be satisfied by any entropic functional candidate to generate non-conventional statistical mechanics. In the present effort we show that the κ\kappa-entropy, recently introduced in literature [G. Kaniadakis, Phys. Rev. E 66, 056125 (2002)], satisfies the Lesche stability condition.Comment: Presented at next2003, Second Sardinian International Conference on News and Expectations in Thermostatistics, Villasimius (Cagliari) Italy, 21st-28th September 2003. In press Physica A (2004). Elsevier LaTeX macros, 10 pages, minor change

    Deformed logarithms and entropies

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    By solving a differential-functional equation inposed by the MaxEnt principle we obtain a class of two-parameter deformed logarithms and construct the corresponding two-parameter generalized trace-form entropies. Generalized distributions follow from these generalized entropies in the same fashion as the Gaussian distribution follows from the Shannon entropy, which is a special limiting case of the family. We determine the region of parameters where the deformed logarithm conserves the most important properties of the logarithm, and show that important existing generalizations of the entropy are included as special cases in this two-parameter class.Comment: Presented at next2003, Second Sardinian International Conference on News and Expectations in Thermostatistics, Villasimius (Cagliari) Italy, 21st-28th September 2003. In press Physica A (2004). Elsevier LaTeX macros, 11 pages, 1 figur

    Stabilities of generalized entropies

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    The generalized entropic measure, which is optimized by a given arbitrary distribution under the constraints on normalization of the distribution and the finite ordinary expectation value of a physical random quantity, is considered and its Lesche stability property (that is different from thermodynamic stability) is examined. A general condition, under which the generalized entropy becomes stable, is derived. Examples known in the literature, including the entropy for the stretched-exponential distribution, the quantum-group entropy, and the kappa-entropy are discussed.Comment: 16 pages, no figure

    Composition law of κ\kappa-entropy for statistically independent systems

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    The intriguing and still open question concerning the composition law of κ\kappa-entropy Sκ(f)=12κi(fi1κfi1+κ)S_{\kappa}(f)=\frac{1}{2\kappa}\sum_i (f_i^{1-\kappa}-f_i^{1+\kappa}) with 0<κ<10<\kappa<1 and ifi=1\sum_i f_i =1 is here reconsidered and solved. It is shown that, for a statistical system described by the probability distribution f={fij}f=\{ f_{ij}\}, made up of two statistically independent subsystems, described through the probability distributions p={pi}p=\{ p_i\} and q={qj}q=\{ q_j\}, respectively, with fij=piqjf_{ij}=p_iq_j, the joint entropy Sκ(pq)S_{\kappa}(p\,q) can be obtained starting from the Sκ(p)S_{\kappa}(p) and Sκ(q)S_{\kappa}(q) entropies, and additionally from the entropic functionals Sκ(p/eκ)S_{\kappa}(p/e_{\kappa}) and Sκ(q/eκ)S_{\kappa}(q/e_{\kappa}), eκe_{\kappa} being the κ\kappa-Napier number. The composition law of the κ\kappa-entropy is given in closed form, and emerges as a one-parameter generalization of the ordinary additivity law of Boltzmann-Shannon entropy recovered in the κ0\kappa \rightarrow 0 limit.Comment: 14 page

    A new one parameter deformation of the exponential function

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    Recently, in the ref. Physica A \bfm{296} 405 (2001), a new one parameter deformation for the exponential function exp{κ}(x)=(1+κ2x2+κx)1/κ;exp{0}(x)=exp(x)\exp_{_{\{{\scriptstyle \kappa}\}}}(x)= (\sqrt{1+\kappa^2x^2}+\kappa x)^{1/\kappa}; \exp_{_{\{{\scriptstyle 0}\}}}(x)=\exp (x), which presents a power law asymptotic behaviour, has been proposed. The statistical distribution f=Z1exp{κ}[β(Eμ)]f=Z^{-1}\exp_{_{\{{\scriptstyle \kappa}\}}}[-\beta(E-\mu)], has been obtained both as stable stationary state of a proper non linear kinetics and as the state which maximizes a new entropic form. In the present contribution, starting from the κ\kappa-algebra and after introducing the κ\kappa-analysis, we obtain the κ\kappa-exponential exp{κ}(x)\exp_{_{\{{\scriptstyle \kappa}\}}}(x) as the eigenstate of the κ\kappa-derivative and study its main mathematical properties.Comment: 5 pages including 2 figures. Paper presented in NEXT2001 Meetin

    Nonlinear gauge transformation for a class of Schroedinger equations containing complex nonlinearities

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    We consider a wide class of nonlinear canonical quantum systems described by a one-particle Schroedinger equation containing a complex nonlinearity. We introduce a nonlinear unitary transformation which permits us to linearize the continuity equation. In this way we are able to obtain a new quantum system obeying to a nonlinear Schroedinger equation with a real nonlinearity. As an application of this theory we consider a few already studied Schroedinger equations as that containing the nonlinearity introduced by the exclusion-inclusion principle, the Doebner-Goldin equation and others. PACS numbers: 03.65.-w, 11.15.-qComment: 3pages, two columns, RevTeX4, no figure

    Kinetical Foundations of Non Conventional Statistics

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    After considering the kinetical interaction principle (KIP) introduced in ref. Physica A {\bf296}, 405 (2001), we study in the Boltzmann picture, the evolution equation and the H-theorem for non extensive systems. The qq-kinetics and the κ\kappa-kinetics are studied in detail starting from the most general non linear Boltzmann equation compatible with the KIP.Comment: 11 pages, no figures. Contribution paper to the proseedings of the International School and Workshop on Nonextensive Thermodynamics and Physical Applications, NEXT 2001, 23-30 May 2001, Cagliari Sardinia, Italy (Physica A

    Nonlinear Transformation for a Class of Gauged Schroedinger Equations with Complex Nonlinearities

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    In the present contribution we consider a class of Schroedinger equations containing complex nonlinearities, describing systems with conserved norm ψ2|\psi|^2 and minimally coupled to an abelian gauge field. We introduce a nonlinear transformation which permits the linearization of the source term in the evolution equations for the gauge field, and transforms the nonlinear Schroedinger equations in another one with real nonlinearities. We show that this transformation can be performed either on the gauge field AμA_\mu or, equivalently, on the matter field ψ\psi. Since the transformation does not change the quantities ψ2|\psi|^2 and FμνF_{\mu\nu}, it can be considered a generalization of the gauge transformation of third kind introduced some years ago by other authors. Pacs numbers: 03.65.-w, 11.15.-qComment: 4pages, two columns, RevTeX4, no figure
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