论文标题

自偶联辐射空间时间中的重力散射

Graviton scattering in self-dual radiative space-times

论文作者

Adamo, Tim, Mason, Lionel, Sharma, Atul

论文摘要

在弯曲的太空时间上构造振幅是一个主要挑战,尤其是当背景具有非恒定曲率时。我们为弯曲的自偶辐射空间时间中的所有树级重力散射幅度提供了公式;这些是手性,无源,渐近平坦的空间,由无效无穷大的自由特征数据确定。这样的太空时间在Twistor理论方面承认了一个优雅的描述,该描述提供了利用其潜在集成性所需的强大工具。树级S-Matrix是根据从Riemann Sphere到Twistor空间的全体形态图的模量空间的积分编写的,其地图的程度与外部重力的螺旋构型相对应。对于MHV领域,我们直接从爱因斯坦 - 希尔伯特(Einstein-Hilbert)的一般相对论的作用中得出幅度,而其他螺旋性构型则来自自然产生功能的家族,并通过了几个一致性检查。自动辐射空间时间中的幅度表现出许多新型特征,这些功能在Minkowski空间中没有,包括尾部效果。由于背景时空中的功能自由度,由于功能自由度而存在残留积分,但是我们的公式比时空扰动理论所期望的要少得多。在高度对称的特殊情况下,例如自偶平面波,可以进一步减少残差积分的数量,从而为散射幅度提供更简单的表达。

The construction of amplitudes on curved space-times is a major challenge, particularly when the background has non-constant curvature. We give formulae for all tree-level graviton scattering amplitudes in curved self-dual radiative space-times; these are chiral, source-free, asymptotically flat spaces determined by free characteristic data at null infinity. Such space-times admit an elegant description in terms of twistor theory, which provides the powerful tools required to exploit their underlying integrability. The tree-level S-matrix is written in terms of an integral over the moduli space of holomorphic maps from the Riemann sphere to twistor space, with the degree of the map corresponding to the helicity configuration of the external gravitons. For the MHV sector, we derive the amplitude directly from the Einstein-Hilbert action of general relativity, while other helicity configurations arise from a natural family of generating functionals and pass several consistency checks. The amplitudes in self-dual radiative space-times exhibit many novel features that are absent in Minkowski space, including tail effects. There remain residual integrals due to the functional degrees of freedom in the background space-time, but our formulae have many fewer such integrals than would be expected from space-time perturbation theory. In highly symmetric special cases, such as self-dual plane waves, the number of residual integrals can be further reduced, resulting in much simpler expressions for the scattering amplitudes.

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