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arXiv 2108.01970gr-qchep-th
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$f(Q)$理论中的量子宇宙学

Quantum Cosmology in $f(Q)$ theory

N. Dimakis, A. Paliathanasis, T. Christodoulakis

摘要:

本文在$f(Q)$宇宙学的背景下,用Dirac方法量子化约束系统,以研究空间平坦的Friedmann-Lemaitre-Robertson-Walker时空.当考虑重合规范时,得到的小超空间系统具有第二类约束。这将量子化过程与典型的惠勒-德威特量子化区别开来,后者适用于只有第一类约束的宇宙学模型(例如广义相对论或$f(R)$引力模型)。我们引入狄拉克括号,找到合适的正则坐标,然后应用正则量子化过程。我们在真空和物质存在下执行此方法:最小耦合标量场和具有线性状态方程的理想流体。我们证明了物质含量的变化显着的量子化过程中,与完美的流体,甚至需要投入使用的分数量子力学的理论,其中的动力的哈密顿量与分形维数的列维飞行。由于$f(Q)$理论和$f(T)$理论在宇宙学研究中具有相同的自由度和动力学约束,本文的分析结果可以应用于$f(T)$遥平行宇宙学。

英文摘要:

We use Dirac's method for the quantization of constrained systems in order to quantize a spatially flat Friedmann-Lemaître-Robertson-Walker spacetime in the context of $f(Q)$ cosmology. When the coincident gauge is considered, the resulting minisuperspace system possesses second class constraints. This distinguishes the quantization process from the typical Wheeler-DeWitt quantization, which is applied for cosmological models where only first class constraints are present (e.g. for models in General Relativity or in $f(R)$ gravity). We introduce the Dirac brackets, find appropriate canonical coordinates and then apply the canonical quantization procedure. We perform this method both in vacuum and in the presence of matter: a minimally coupled scalar field and a perfect fluid with a linear equation of state. We demonstrate that the matter content changes significantly the quantization procedure, with the perfect fluid even requiring to put in use the theory of fractional Quantum Mechanics in which the power of the momentum in the Hamiltonian is associated with the fractal dimension of a Lévy flight. The results of this analysis can be applied in $f(T)$ teleparallel cosmology, since $f(Q)$ and $f(T)$ theories have the same degrees of freedom and same dynamical constraints in cosmological studies.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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