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arXiv 2402.01487gr-qchep-th
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非共形引力波

Disformal gravitational waves

Jibril Ben Achour, Mohammad Ali Gorji, Hugo Roussille

AI总结:

本文针对非共形变换下引力波性质可能改变的问题,给出其充要条件,论证不依赖坐标且适用于完全非线性时空,通过示例展示非线性水平下非共形变换可产生张量引力波,该效应在线性微扰理论中易被忽略。

摘要:

与共形变换不同,非共形变换可改变时空几何的主零方向。因此,根据引力波(GW)探测器最小耦合的参考系,GW的性质在非共形变换下可能发生变化。本文给出了判断GW在非共形变换下是否变化的充要条件。我们的论证不依赖坐标,可应用于完全非线性水平的任意时空几何。作为示例,我们展示了仅允许无剪切平行输运参考系的无质量爱因斯坦-标量引力的精确辐射解,被映射为不具有任何无剪切平行输运参考系的非共形几何。这种辐射几何及其非共形对应体提供了一个具体示例,说明在完全非线性水平下通过非共形变换产生张量GW的可能性。这种非线性效应在通常的线性微扰理论中可能被完全忽略。

英文摘要:

Contrary to conformal transformations, disformal transformations can change the principal null directions of a spacetime geometry. Thus, depending on the frame a gravitational wave (GW) detector minimally couples to, the properties of GWs may change under a disformal transformation. In this paper, we provide necessary and sufficient conditions which determine whether GWs change under disformal transformations or not. Our argument is coordinate-independent and can be applied to any spacetime geometry at the fully non-linear level. As an example, we show that an exact radiative solution of massless Einstein-scalar gravity which admits only shear-free parallel transported frame is mapped to a disformed geometry which does not possess any shear-free parallel transported frame. This radiative geometry and its disformed counterpart provide a concrete example of the possibility to generate tensorial GWs from a disformal transformation at the fully non-linear level. This type of non-linear effect can be completely overlooked in the usual linear perturbation theory.

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