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Power laws are disguised Boltzmann laws

机译:幂律是伪装的玻尔兹曼定律

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摘要

Using a previously introduced model on generalized Lotka-Volterra dynamics together with some recent results for the solution of generalized Langevin equations, we derive analytically the equilibrium mean field solution for the probability distribution of wealth and show that it has two characteristic regimes. For large values of wealth, it takes the form of a Pareto style power law. For small values of wealth, w less than or equal to w(m), the distribution function tends sharply to zero. The origin of this law lies in the random multiplicative process built into the model. Whilst such results have been known since the time of Gibrat, the present framework allows for a stable power law in an arbitrary and irregular global dynamics, so long as the market is "fair", i.e., there is no net advantage to any particular group or individual. We further show that the dynamics of relative wealth is independent of the specific nature of the agent interactions and exhibits a universal character even though the total wealth may follow an arbitrary and complicated dynamics. In developing the theory, we draw parallels with conventional thermodynamics and derive for the system some new relations for the "thermodynamics" associated with the Generalized Lotka-Volterra type of stochastic dynamics. The power law that arises in the distribution function is identified with new additional logarithmic terms in the familiar Boltzmann distribution function for the system. These are a direct consequence of the multiplicative stochastic dynamics and are absent for the usual additive stochastic processes. [References: 22]
机译:使用先前介绍的广义Lotka-Volterra动力学模型,以及对广义Langevin方程求解的一些最新结果,我们分析得出财富概率分布的均衡平均场解,并表明它具有两个特征形式。对于大量的财富,它采用帕累托式幂律的形式。对于较小的财富值,w小于或等于w(m),分布函数会急剧趋于零。该法则的起源在于模型中内置的随机乘法过程。尽管自吉布拉特时代以来就已经知道了这样的结果,但只要市场是“公平的”,即任何特定群体都没有净利益,则本框架允许在任意和不规则的全球动态中建立稳定的幂律。或个人。我们进一步证明,相对财富的动态独立于主体相互作用的特定性质,即使总财富可能遵循任意复杂的动态,它也具有普遍性。在发展该理论时,我们与传统的热力学有相似之处,并为系统推导了与广义Lotka-Volterra类型的随机动力学有关的“热力学”的一些新关系。分布函数中出现的幂定律在系统熟悉的Boltzmann分布函数中用新的附加对数项来标识。这些是乘法随机动力学的直接结果,对于通常的加法随机过程是不存在的。 [参考:22]

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