再来看看相互作用的Chaplygin气体

S. Saha, Saumya Ghosh, S. Gangopadhyay
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引用次数: 4

摘要

探讨了用常状态方程考虑Chaplygin气体与正压流体相互作用的意义。这项工作的独特之处在于假设相互作用$Q \propto H\rho_d$,能量密度和压力的解析表达式已经根据超几何$_2\text{F}_1$函数导出。值得一提的是,Zhang和Zhu在2006年考虑了一个相互作用的Chaplygin气体模型,然而,假设相互作用正比于$H$乘以Chaplygin气体和尘埃的能量密度之和,则无法确定连续性方程的解析解。我们的模型可以成功地解释从早期的减速阶段到现在的宇宙加速阶段的转变。通过试错法对模型自由参数的任意选择表明,在最近的观测数据中,$w_m=0$和$w_m=-\frac{1}{3}$明显优于$w_m=\frac{1}{3}$。有趣的是,目前的模型也将暗能量的跃迁纳入幻影域,然而,未来的减速是被禁止的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Interacting Chaplygin gas revisited
The implications of considering interaction between Chaplygin gas and a barotropic fluid with constant equation of state have been explored. The unique feature of this work is that assuming an interaction $Q \propto H\rho_d$, analytic expressions for the energy density and pressure have been derived in terms of the Hypergeometric $_2\text{F}_1$ function. It is worthwhile to mention that an interacting Chaplygin gas model was considered in 2006 by Zhang and Zhu, nevertheless, analytic solutions for the continuity equations could not be determined assuming an interaction proportional to $H$ times the sum of the energy densities of Chaplygin gas and dust. Our model can successfully explain the transition from the early decelerating phase to the present phase of cosmic acceleration. Arbitrary choice of the free parameters of our model through trial and error show at recent observational data strongly favors $w_m=0$ and $w_m=-\frac{1}{3}$ over the $w_m=\frac{1}{3}$ case. Interestingly, the present model also incorporates the transition of dark energy into the phantom domain, however, future deceleration is forbidden.
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