Scalar cosmological perturbations from quantum gravitational entanglement

IF 3.7 3区 物理与天体物理 Q2 ASTRONOMY & ASTROPHYSICS Classical and Quantum Gravity Pub Date : 2024-08-20 DOI:10.1088/1361-6382/ad6f67
Alexander F Jercher, Luca Marchetti and Andreas G A Pithis
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Abstract

A major challenge at the interface of quantum gravity (QG) and cosmology is to explain the emergence of the large-scale structure of the Universe from Planck scale physics. In this letter, we extract the dynamics of scalar isotropic cosmological perturbations from full QG, as described by the causally complete Barrett–Crane group field theory (GFT) model. From the perspective of the underlying QG theory, cosmological perturbations are represented as nearest-neighbor two-body entanglement of GFT quanta. Their effective dynamics is obtained via mean-field methods and described relationally with respect to a causally coupled physical Lorentz frame. We quantitatively study these effective dynamical equations and show that at low energies they are perfectly consistent with those of general relativity, while for trans-Planckian scales quantum effects become important. These results therefore not only provide crucial insights into the potentially purely quantum gravitational nature of cosmological perturbations, but also offer rich phenomenological implications for the physics of the early Universe.
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来自量子引力纠缠的标量宇宙学扰动
量子引力(QG)与宇宙学交界处的一大挑战是如何从普朗克尺度物理学解释宇宙大尺度结构的出现。在这封信中,我们从完全量子引力(QG)中提取了标量各向同性宇宙学扰动的动力学,正如因果完整的巴雷特-克兰群场论(GFT)模型所描述的那样。从基础 QG 理论的角度来看,宇宙学扰动被表示为 GFT 量子的最近邻二体纠缠。它们的有效动力学是通过均场方法获得的,并与因果耦合物理洛伦兹框架相关联地进行了描述。我们对这些有效动力学方程进行了定量研究,结果表明,在低能量时,它们与广义相对论的方程完全一致,而在跨普朗克尺度时,量子效应变得非常重要。因此,这些结果不仅为宇宙学扰动的潜在纯量子引力性质提供了重要见解,还为早期宇宙物理学提供了丰富的现象学意义。
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来源期刊
Classical and Quantum Gravity
Classical and Quantum Gravity 物理-天文与天体物理
CiteScore
7.00
自引率
8.60%
发文量
301
审稿时长
2-4 weeks
期刊介绍: Classical and Quantum Gravity is an established journal for physicists, mathematicians and cosmologists in the fields of gravitation and the theory of spacetime. The journal is now the acknowledged world leader in classical relativity and all areas of quantum gravity.
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