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arXiv 2012.13960gr-qc
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$f(R)$宇宙学中通过标量子自发衰变的原初再加热

Primordial reheating in $f(R)$ cosmology by spontaneous decay of scalarons

Arun Mathew, Malay K. Nandy

AI总结:

本研究基于$f(R)$引力模型,结合海森堡不确定性原理构建原初再加热图景,分析标量子场能量驱动的粒子产生过程,给出暴胀、预热及热化阶段的时长与温度等关键参数,且所有估计仅由标量子质量单参数推导。

摘要:

我们采用一种可产生暴胀阶段的可行$f(R)$引力模型,以研究随后的再加热阶段,该阶段源于以标量子场能量为代价的粒子产生。由于量子力学预计在粒子产生中起主导作用,我们构建了一种符合海森堡不确定性原理的合理再加热图景,该原理对构形空间中产生的粒子施加了约束。我们表明,只要标量子场中可用的能量足以填满整个构形空间,粒子的能量密度就会增长,达到一个能实现高效再加热的最大值。超过这个最大值后,可用能量不足以填满整个构形空间,导致能量密度下降。\n我们进一步发现,在持续约$10^7 \t_{\rm P}$(普朗克时间)的暴胀阶段,尽管粒子不断产生,但能量密度的增长可以忽略不计。随后的再加热阶段持续约$10^{11} \t_{\rm P}$,它以一个持续约$10^5 \t_{\rm P}$的明确定义的预热阶段开始,随后过渡到热化阶段。热化开始时的温度为$T_{\rm th}\sim 10^{12}$ GeV,而再加热温度估计为$T_{r}\sim10^{13}$ GeV。重要的是,这些估计值仅由单个参数即标量子质量$M\sim10^{-5} \\\\\\ M_{\rm P}$(普朗克质量)推导得出。

英文摘要:

We employ a viable $f(R)$ gravity model capable of giving an inflationary phase in order to study the subsequent reheating phase due to particle creation at the expense of energy in the scalaron field. Since quantum mechanics is expected to play a dominant role in particle creation, we formulate a plausible scenario of reheating obeying Heisenberg's uncertainty principle that imposes constraints on the particles created in the configuration space. We show that, so long as the energy available in the scalaron field is sufficient to populate the entire configuration space, the energy density of the particles grows, attaining a maximum value giving an efficient reheating. Beyond this maximum, the available energy becomes insufficient to populate the entire configuration space leading to a declining energy density. We further find that there is a negligible growth of energy density in the inflationary phase that lasts for $\sim 10^7 \, t_{\rm P}$, although particles are constantly created in this phase. The subsequent reheating phase spans for $\sim10^{11} \, t_{\rm P}$ and it begins with a well-defined preheating stage lasting for $\sim 10^{5} \, t_{\rm P}$, making a cross-over to a thermilization regime. The temperature at the beginning of the thermilization is found to be $T_{\rm th}\sim 10^{12}$ GeV, whereas the reheating temperature is estimated as $T_{r}\sim10^{13}$ GeV. Importantly, these estimates follow from a single parameter, the scalaron mass, $M\sim10^{-5} \, M_{\rm P}$.

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