The numerical waveforms produced by SpEC are made dimensionless by scaling by the Christodoulou mass computed early in the simulation. This value should be treated as Lorentz invariant. This PR only needs to change the transformation for WaveformModes and WaveformGrid objects because the AsymptoticBondiData interface assumes the quantites are dimensionful (or that the Christodoulou mass is Lorentz invariant).
The primary argument for this is from @moble. The following plot shows the value of the Christodoulou mass over the course of the simulation along with a prediction from arxiv:gr-qc/0107080. Here we have the Lev6 mass value (averaged between T=2000 and 5000), and added the integrated change in mass.
Comparing transformed waveforms with and without treating the Christodoulou mass as Lorentz invariant shows that the difference is equal to applied gamma factor appropriate to each waveform quantity.
The numerical waveforms produced by SpEC are made dimensionless by scaling by the Christodoulou mass computed early in the simulation. This value should be treated as Lorentz invariant. This PR only needs to change the transformation for
WaveformModes
andWaveformGrid
objects because theAsymptoticBondiData
interface assumes the quantites are dimensionful (or that the Christodoulou mass is Lorentz invariant).The primary argument for this is from @moble. The following plot shows the value of the Christodoulou mass over the course of the simulation along with a prediction from arxiv:gr-qc/0107080. Here we have the Lev6 mass value (averaged between T=2000 and 5000), and added the integrated change in mass.