论文标题
在Axion $ f(r)$ GRAVITY中与早期和晚期的深色能源时期的通货膨胀统一
Unifying of Inflation with Early and Late Dark Energy Epochs in Axion $F(R)$ Gravity
论文作者
论文摘要
我们提供了$ f(r)$重力的理论模型,在这种模型中,在存在宇宙暗物质成分的作用的光轴粒子的情况下,可以以统一的通货膨胀,早期和晚期的黑暗能量时代来描述。特别是,早期现象学以$ r^2 $术语为主,而其他术语的存在$ f(r)$确保出现早期和迟到的黑暗能源时代。通货膨胀现象学与Planck 2018通货膨胀数据兼容,而迟到的黑暗能源时代与Planck 2018对宇宙学参数的约束兼容。此外,该模型还展示了早期的黑暗能源时代,$ z \ sim 2.5 $大约,其次是减速时代,其起点约为$ z \ sim 1.5 $,然后又是RedShifts $ z \ sim 0.5 $的后期深色能源时代,持续约50亿年。我们模型的一个值得注意的特征是,深色能源时代至少在红移间隔$ z = [0,10] $的情况下没有暗能量振荡。此外,我们还讨论了与$ z \ sim 2.34 $的观察数据相关的几个功能,文献中存在红移复杂的观察数据。此外,本文的末尾介绍了用Python 3编写的暗能量现象学的数值代码。最后,该模型具有另一个有趣的特征,在红移间隔$ z \ sim [2,2.6] $中突然跳高了哈勃速率的价值,其中其值突然增加,然后降低直到$ z \ sim 0 $。
We provide a theoretical model of $F(R)$ gravity in which it is possible to describe in a unified way inflation, an early and a late dark energy era, in the presence of a light axion particle which plays the role of the dark matter component of the Universe. Particularly, the early-time phenomenology is dominated by an $R^2$ term, while the presence of the other terms $f(R)$ ensure the occurrence of the early and late-time dark energy eras. The inflationary phenomenology is compatible with the Planck 2018 data for inflation, while the late-time dark energy era is compatible with the Planck 2018 constraints on the cosmological parameters. Also, the model exhibits an early dark energy era, at $z\sim 2.5$ approximately, followed by a deceleration era, which starts at approximately $z\sim 1.5$, which in turn is followed by a late-time dark energy era for redshifts $z\sim 0.5$, which lasts for approximately 5 billion years up to present time. A notable feature of our model is that the dark energy era is free from dark energy oscillations, at least in the redshift interval $z=[0,10]$. In addition, we also discuss several features related to observational data at $z\sim 2.34$, at which redshift intricate observational data exist in the literature. Moreover, the numerical code for the dark energy phenomenology, written in Python 3, is presented in the end of the article. Finally, the model has another interesting characteristic, a sudden jump of the value of the Hubble rate in the redshift interval $z\sim [2,2.6]$ where its value suddenly increases and then decreases until $z\sim 0$.