帕拉蒂尼公式中带有 $R^2$ 项的最小耦合 $β$ 指数通货膨胀

Nilay Bostan, Rafid H. Dejrah
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引用次数: 0

摘要

我们重点研究了$\beta$-指数势模型的膨胀预测,其中膨胀子是划分维度外大小的场的代表。由于它为研究高能物理提供了一个动机良好的起点,我们在帕拉蒂尼引力中加入了一个$R^2$项。此外,在暴胀之后,膨胀子围绕暴胀势的最小值振荡,并重新加热宇宙。这发生在再热阶段,此时膨胀子衰变为标准模型粒子,填充了整个宇宙。我们通过采用不同的再热温度方案来扩展我们的研究,考虑再热对暴胀观测值的影响。假设暴胀后的标准热历史,我们展示了帕拉蒂尼$R^2$引力中具有最小耦合的$\beta$-指数势的暴胀预言,$n_s, r, \mathrm{d}n_s/\mathrm{d}\ln k$。此外,这项工作还考虑了来自各种观测的不同约束,如BICEP/Keck、Planck 2018,以及未来CMB实验可能达到的可探测灵敏度:CMB-S4和LiteBIRD。我们指出,我们的结果与 LiteBIRD/Planck 和 CMB-S4 的最新数据和未来灵敏度预测一致。最后,本研究的结果突出了我们的模型的可行性,即使在存在未来可实现置信水平限值所预期的更严格约束的情况下也是如此。
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Minimally coupled $β$-exponential inflation with an $R^2$ term in the Palatini formulation
We focus on the inflationary predictions of $\beta$-exponential potential models, in which the inflaton is a representation of the field delineating the size of extra-dimension. Since it offers a well-motivated starting point for the study of physics at very high energies, we incorporate an $R^2$ term in the Palatini gravity. In addition, afterward the inflation, the inflaton oscillates about the minimum of the inflation potential, and reheats the universe. This occurs during the reheating phase, at which the inflaton decays into the standard model particles, which fill the universe. We extend our examination by considering the reheating effects on inflationary observables by employing the different scenarios of the reheat temperature. Supposing the standard thermal history after inflation, we display the inflationary predictions, $n_s, r, \mathrm{d}n_s/\mathrm{d}\ln k$ of $\beta$-exponential potential with minimal coupling in Palatini $R^2$ gravity. Also, different kinds of constraints from a variety of observations, such as BICEP/Keck, Planck 2018, as well as future possible detectable sensitivities that might be reached by CMB experiments: CMB-S4 and LiteBIRD are taken into account in this work. We indicate that our results are consistent with both the latest data and the future sensitivity forecasts of LiteBIRD/Planck and CMB-S4. Finally, the results in this study highlight the viability of our model even in the case of the existence of more stringent constraints expected from future achievable confidence level limits.
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