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arXiv 2302.04285gr-qc
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圈宇宙学中一族微分同胚不变的度量-仿射作用量

A diffeomorphism invariant family of metric-affine actions for loop cosmologies

Adrià Delhom, Gonzalo J. Olmo, Parampreet Singh

AI总结:

本文研究了圈量子宇宙学模型与度量-仿射有效作用量的关系,发现一族3参数f(R)理论能准确近似LQC、mLQC-II及mLQC-I反弹后的有效动力学,且非微扰效应由对数修正普遍编码。

摘要:

在圈量子宇宙学(LQC)中,大爆炸奇点通常通过大反弹得到解决。即使在使用修正的哈密顿约束量子化方案(如 mLQC-I 和 mLQC-II)时,这一特征依然成立。虽然后者描述的有效描述与标准 LQC 定性相似,但前者描述了一种非对称演化,即使在没有势的情况下,在反弹前也会出现一个涌现的普朗克尺度德西特相。我们考虑了这些正则量子化的非奇异模型与基于几何描述的有效作用量之间的潜在关系。我们发现了一个 3 参数族的度量-仿射 f(R) 理论,它在所有区域准确近似 LQC 和 mLQC-II 的有效动力学,并在反弹后阶段近似 mLQC-I。通过在反弹点强制等价性固定其中两个参数,相关可观测量的背景演化只需一个自由参数即可拟合。可以看到,这些圈宇宙学的非微扰效应普遍由一个仅依赖于模型反弹曲率的对数修正来编码。此外,我们发现该自由参数的最佳拟合值可以非常近似地用这三个模型底层量子描述的基本参数来表示。最佳拟合值可以简单方式用反弹密度写出,且每个模型的值通过仅包含 Barbero-Immirzi 参数的比例关系相互关联。

英文摘要:

In loop quantum cosmology (LQC) the big bang singularity is generically resolved by a big bounce. This feature holds even when modified quantization prescriptions of the Hamiltonian constraint are used such as in mLQC-I and mLQC-II. While the later describes an effective description qualitatively similar to that of standard LQC, the former describes an asymmetric evolution with an emergent Planckian de-Sitter pre-bounce phase even in the absence of a potential. We consider the potential relation of these canonically quantized non-singular models with effective actions based on a geometric description. We find a 3-parameter family of metric-affine $f(\mathcal{R})$ theories which accurately approximate the effective dynamics of LQC and mLQC-II in all regimes and mLQC-I in the post-bounce phase. Two of the parameters are fixed by enforcing equivalence at the bounce, and the background evolution of the relevant observables can be fitted with only one free parameter. It is seen that the non-perturbative effects of these loop cosmologies are universally encoded by a logarithmic correction that only depends on the bounce curvature of the model. In addition, we find that the best fit value of the free parameter can be very approximately written in terms of fundamental parameters of the underlying quantum description for the three models. The values of the best fits can be written in terms of the bounce density in a simple manner, and the values for each model are related to one another by a proportionality relation involving only the Barbero-Immirzi parameter.

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