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A general theory of linear cosmological perturbations: scalar-tensor and vector-tensor theories

机译:线性宇宙微扰的一般理论:标量张量和矢量张量理论

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摘要

We present a method for parametrizing linear cosmological perturbations of theories of gravity, around homogeneous and isotropic backgrounds. The method is sufficiently general and systematic that it can be applied to theories with any degrees of freedom (DoFs) and arbitrary gauge symmetries. In this paper, we focus on scalar tensor and vector-tensor theories, invariant under linear coordinate transformations. In the case of scalar-tensor theories, we use our framework to recover the simple parametrizations of linearized Horndeski and "Beyond Horndeski" theories, and also find higher-derivative corrections. In the case of vector-tensor theories, we first construct the most general quadratic action for perturbations that leads to second-order equations of motion, which propagates two scalar IDoFs. Then we specialize to the case in which the vector field is time-like (a la Einstein-Aether gravity), where the theory only propagates one scalar DoE. As a result, we identify the complete forms of the quadratic actions for perturbations, and the number of free parameters that need to be defined, to cosmologically characterize these two broad classes of theories.
机译:我们提出了一种在均匀和各向同性的背景下参数化引力理论的线性宇宙微扰的方法。该方法具有足够的通用性和系统性,可以应用于具有任何自由度(DoF)和任意规范对称性的理论。在本文中,我们集中在线性坐标变换下不变的标量张量和矢量张量理论。就标量张量理论而言,我们使用我们的框架来恢复线性化Horndeski和“ Beyond Horndeski”理论的简单参数化,并找到更高导数的校正。在矢量张量理论的情况下,我们首先为扰动构造最一般的二次动作,从而导致运动的二阶运动方程式传播两个标量IDoF。然后,我们专门研究矢量场类似于时间(la Einstein-Aether引力)的情况,其中该理论仅传播一个标量DoE。结果,我们确定了扰动的二次动作的完整形式,以及需要定义的自由参数的数量,以便从宇宙学角度表征这两种广泛的理论。

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