所有的顺序引力波形式来自散射幅度
Tim Adamo1, Andrea Cristofoli1, Anton Ilderton2
1School of Mathematics and Maxwell Institute for Mathematical Sciences, University of Edinburgh, Edinburgh, EH9 3FD, United Kingdom.
Physical review letters
|July 21, 2023
概括
这项研究使用强场振幅计算了来自大质量粒子散射的引力波形在精确的引力平面波上. 结果揭示了无限的Minkowskian后贡献和尾部效应,与弱场近似不同.
科学领域:
- 引力物理 引力物理
- 一般相对论一般相对论.
- 高能粒子的散射是高能粒子的散射.
背景情况:
- 波形是辐射过程中的经典可观测物,通常使用弱场近似计算,如后牛顿式或后明科夫斯基式扩张.
- 散射幅度是计算这些波形在弱场极限中的标准工具.
研究的目的:
- 计算由大质量粒子散射在确切的引力平面波上产生的波形.
- 探索强场效应超出传统近似的范围.
- 将引力结果与类似的电磁现象进行比较.
主要方法:
- 使用强场散射幅度. 使用强场散射幅度.
- 将引力平面波视为爱因斯坦真空方程的精确非线性解.
- 计算大质量粒子散射的波形.
主要成果:
- 计算的波形包括无限数量的Minkowskian后贡献.
- 尾部效应存在于波形中.
- 在电磁学中得出类似的结果并对比.
结论:
- 强场散射幅度提供了一个更完整的描述从引力平面波的波形.
- 这种方法捕捉了诸如无限后明科夫斯基式项和尾巴效应等现象,这些现象被弱场近似错过了.
- 该研究为了解强引力场中的辐射过程及其电磁对应物提供了一个框架.
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