2019
DOI: 10.1016/j.physa.2018.10.044
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Burr type-XII as a superstatistical stationary distribution

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Cited by 8 publications
(3 citation statements)
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“…Thereby, the overall probability defines the superstatistics of Gaussian statistics corresponding to different diffusivity packets. The above overall probability (Equation (4)) was analyzed in different scenarios in diffusion theory: (i) p(D) as a χ 2 gamma distribution in the context of random diffusivity, to compare with the diffusive diffusivity model [44], or to describe the movement of many individual small organisms that move with different diffusivities [54]; (ii) p(N) as a χ 2 -inverse gamma distribution that depends on particle size to investigate the aggregation and fragmentation process in the context of Laplace diffusion [50]; (iii) p(D) as a stretched exponential to construct a stretched Gaussian diffusion [17,55]; (iv) p(D) Lévy distribution to construct a Lévy process caused by large fluctuations in environment [52]; (v) p(β ∝ 1/T) as a Mittag-Leffler function to construct generalized Maxwell-Boltzmann distributions [56] and other generalized distributions [57,58], even as truncated-Mittag-Leffler function [59], which was applied in the analysis of the time series of oil price.…”
Section: From Log-normal Superstatistics To Brownian Yet Non-gaussianmentioning
confidence: 99%
“…Thereby, the overall probability defines the superstatistics of Gaussian statistics corresponding to different diffusivity packets. The above overall probability (Equation (4)) was analyzed in different scenarios in diffusion theory: (i) p(D) as a χ 2 gamma distribution in the context of random diffusivity, to compare with the diffusive diffusivity model [44], or to describe the movement of many individual small organisms that move with different diffusivities [54]; (ii) p(N) as a χ 2 -inverse gamma distribution that depends on particle size to investigate the aggregation and fragmentation process in the context of Laplace diffusion [50]; (iii) p(D) as a stretched exponential to construct a stretched Gaussian diffusion [17,55]; (iv) p(D) Lévy distribution to construct a Lévy process caused by large fluctuations in environment [52]; (v) p(β ∝ 1/T) as a Mittag-Leffler function to construct generalized Maxwell-Boltzmann distributions [56] and other generalized distributions [57,58], even as truncated-Mittag-Leffler function [59], which was applied in the analysis of the time series of oil price.…”
Section: From Log-normal Superstatistics To Brownian Yet Non-gaussianmentioning
confidence: 99%
“…Поиск распределений, заменяющих логнормальное распределение и объединяющих в себе свойства степенного и логнормального распределений, ведется на протяжении нескольких десятилетий (см., например, (Champernowne, 1956;Ghosh and Basu, 2019;Sánchez, 2019)). Аналитически простую двухпараметрическую модель PC, дающую широкий диапазон асимметрий, можно получить путем обобщения представленных в…”
Section: модель кривой паретоunclassified
“…The search for distributions that replace the lognormal distribution and combine the properties of the power-series distribution and lognormal distribution has been going on for several decades (for example, see (Champernowne, 1956;Ghosh and Basu, 2019;Sánchez, 2019)). An analytically simple two-parameter PC model that gives a wide range of asymmetries can be obtained by generalizing the single-parameter PCs presented in Table 1 (Antoniou et al, 2004):…”
Section: The Pareto Curve Modelmentioning
confidence: 99%