期刊
PHYSICAL REVIEW D
卷 103, 期 12, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.103.123021
关键词
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资金
- National Key Research and Development Program of China [2020YFC2201503]
- National Natural Science Foundation of China [11675143, 11675145, 11705053, 11975203, 12035005]
- Zhejiang Provincial Natural Science Foundation of China [LR21A050001, LY20A050002]
- Fundamental Research Funds for the Provincial Universities of Zhejiang in China [RFA2019015]
- Japan Society for the Promotion of Science [17H02890, 17H06359]
- World Premier International Research Center Initiative, MEXT, Japan
- Baylor University through the Baylor University Physics graduate program
This paper systematically studies the generation and propagation of gravitational waves, introducing three scales to describe their characteristics and discussing the detection conditions, approximations, and backreaction scenarios. By properly selecting gauge conditions, the research can be significantly simplified to determine the motion properties and effects of gravitational waves in different scenarios.
In this paper, we systematically study gravitational waves (GWs) first produced by remote compact astrophysical sources and then propagating in our inhomogeneous Universe through cosmic distances, before arriving at detectors. To describe such GWs properly, we introduce three scales, lambda, L-c, and L, denoting, respectively, the typical wavelength of GWs, the scale of the cosmological perturbations, and the size of the observable Universe. For GWs to be detected by the current and foreseeable detectors, the condition lambda << L-c << L holds. Then, such GWs can be approximated as high-frequency GWs and be well separated from the background gamma(mu nu) by averaging the spacetime curvatures over a scale l, where lambda << L << L-c , and g(mu nu) = gamma(mu nu) + epsilon h(mu nu) with h(mu nu) denoting the GWs. In order for the backreaction of the GWs to the background spacetimes to be negligible, we must assume that vertical bar h(mu nu)vertical bar << 1, in addition to the condition epsilon << 1, which are also the conditions for the linearized Einstein field equations for h(mu nu) to be valid. Such studies can be significantly simplified by properly choosing gauges, such as the spatial, traceless, and Lorenz gauges. We show that these three different gauge conditions can be imposed simultaneously, even when the background is not a vacuum, as long as the high-frequency GW approximation is valid. However, to develop the formulas that can be applicable to as many cases as possible, in this paper we first write down explicitly the linearized Einstein field equations by imposing only the spatial gauge. Then, applying these formulas together with the geometrical optics approximation to such GWs, we find that they still move along null geodesics and its polarization bivector is parallel transported, even when both the cosmological scalar and tensor perturbations are present. In addition, we also calculate the gravitational integrated Sachs-Wolfe effects due to these two kinds of perturbations, whereby the dependences of the amplitude, phase, and luminosity distance of the GWs on these perturbations are read out explicitly.
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