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arXiv 2210.03348astro-ph.CO
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利用CMB各向异性对早期暗能量相变的约束

Constraints on the phase transition of Early Dark Energy with the CMB anisotropies

Shintaro Hayashi, Teppei Minoda, Kiyotomo Ichiki

AI总结:

本文研究早期暗能量相变产生的等曲率扰动对CMB的影响,发现其幅度被约束在绝热模式的1%-2%以内,无法有效缓解哈勃张力。

摘要:

早期暗能量(EDE)模型在近期哈勃张力问题的背景下引起了关注。本文通过考虑由在复合阶段附近衰变的EDE所产生的新的密度涨落来扩展这些模型。我们求解了在EDE相变时产生的暗能量流体密度扰动作为等曲率扰动的演化。假设等曲率模式由幂律功率谱表征,并且与标准绝热模式不相关,我们计算了CMB角功率谱。通过使用马尔可夫链蒙特卡洛方法将其与Planck数据进行比较,我们得到了与零一致的EDE参数值,以及在68%置信水平下H0=67.56^{+0.65}_{-0.66} km s^{-1} Mpc^{-1}。该H0值与ΛCDM模型中的Planck值H0=67.36±0.54 km s^{-1} Mpc^{-1}几乎相同,CMB与Ia型超新星观测之间仍存在约3.5σ的张力。结合CMB透镜、BAO、超新星和SH0ES数据集,我们发现在68%置信水平下H0=68.94^{+0.47}_{-0.57} km s^{-1} Mpc^{-1}。由EDE相变诱导的涨落幅度被约束为小于绝热模式幅度的1%至2%。这个幅度非常小,以至于这种非标准涨落无法出现在CMB角谱中。总之,由我们最简单的EDE相变模型诱导的等曲率涨落不能很好地解释哈勃张力。

英文摘要:

Early dark energy (EDE) models have attracted attention in the context of the recent problem of the Hubble tension. Here we extend these models by taking into account the new density fluctuations generated by the EDE which decays around the recombination phase. We solve the evolution of the density perturbations in dark energy fluid generated at the phase transition of EDE as isocurvature perturbations. Assuming that the isocurvature mode is characterized by a power-law power spectrum and is uncorrelated with the standard adiabatic mode, we calculate the CMB angular power spectra. By comparing them to the Planck data using the Markov-Chain Monte Carlo method, we obtained zero-consistent values of the EDE parameters and $H_0=67.56^{+0.65}_{-0.66}~\mathrm{km} \, \mathrm{s}^{-1} \mathrm{Mpc}^{-1}$ at $68 \%$ CL. This $H_0$ value is almost the same as the Planck value in the $Λ$CDM model, $H_0=67.36 \pm 0.54~\mathrm{km} \, \mathrm{s}^{-1} \mathrm{Mpc}^{-1}$, and there is still a $\sim 3.5 σ$ tension between the CMB and Type Ia supernovae observations. Including CMB lensing, BAO, supernovae and SH0ES data sets, we find $H_0=68.94^{+0.47}_{-0.57}~\mathrm{km} \, \mathrm{s}^{-1} \mathrm{Mpc}^{-1}$ at $68 \%$ CL. The amplitude of the fluctuations induced by the phase transition of the EDE is constrained to be less than $1$--$2$ percent of the amplitude of the adiabatic mode. This is so small that such non-standard fluctuations cannot appear in the CMB angular spectra. In conclusion, the isocurvature fluctuations induced by our simplest EDE phase transition model do not explain the Hubble tension well.

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