论文标题
具有非扩展统计的血浆振荡的简化计算
Simplified calculations of plasma oscillations with non-extensive statistics
论文作者
论文摘要
我们使用非Xttendition分布的指数参数化来计算遵守非xtentgendentive统计的电子气体中的介电常数。如我们所示,指数参数化允许我们以一种直接的方式进行此类计算,绕过从积分表和/或数值方法获得的复杂公式的使用。出于说明目的,我们首先将方法应用于电子气体超层次性极限中的介电常数和相应的色散关系,并验证它以简单的方式使用了其他作者使用非xtxentive分布的标准参数化获得了先前由其他作者获得的结果。本着同样的精神,我们重新审视了在高频限制下对非相关气体的相同数量的计算,以前是由利马,席尔瓦和桑托斯先前对此进行的,然后由陈和李修订。我们自己的结果与陈和李获得的结果一致。为了完整性,我们还应用了该方法在非权利主义情况下的低频限制,DAI,Chen和Li先前在流等离子体不稳定性的背景下已考虑。我们讨论在每种情况下获得的结果的一些特征及其对通用无Xtentive数量的术语的解释,例如Debye长度$λ_{d}^{(q)} $,Plasma频率$ $ $ω_{p}^{(q)} $和Ultra-Relativistic频率$ $ $ $ω^^{Q)在限制中,$ q \ rightarrow 1 $此类数量减少了其经典价值,并且复制了分散关系的经典结果。
We use the exponential parametrization of the nonextensive distribution to calculate the dielectric constant in an electron gas obeying the nonextensive statistics. As we show, the exponential parametrization allows us to make such calculations in a straightforward way, bypassing the use of intricate formulas obtained from integral tables and/or numerical methods. For illustrative purposes, we apply first the method to the calculation of the permittivity and the corresponding dispersion relation in the ultrarelativistic limit of the electron gas, and verify that it reproduces in a simple way the results that had been obtained previously by other authors using the standard parametrization of the nonextensive distribution. In the same spirit we revisit the calculation of the same quantities for a non-relativistic gas, in the high frequency limit, which has been previously carried out, first by Lima, Silva and Santos, and subsequently revised by Chen and Li. Our own results agree with those obtained by Chen and Li. For completeness, we also apply the method the low frequency limit in the non-relativistic case, which has been previously considered by Dai, Chen and Li in the context of the stream plasma instability. We discuss some features of the results obtained in each case and their interpretation of terms of generalized nonextensive quantities, such as the Debye length $λ_{D}^{(q)}$, the plasma frequency $ω_{p}^{(q)}$ and the ultra-relativistic frequency $Ω^{(q)}_{e,rel}$. In the limit $q \rightarrow 1$ such quantities reduce to their classical value and the classical result of the dispersion relations are reproduced.