All WaveformDataPieces needed to evaluate all modes with a fixed value of ell.
For m=0 modes we model the real and imaginary parts separately. For m>0, we model the real and imaginary parts of X_pm^{ell, m} = frac{1}{2}( h^{ell, m} pm h^{ell, -m} ) where this h is in the coorbital frame. (see https://arxiv.org/abs/1705.07089)
Definition at line 149 of file LALSimIMRPrecessingNRSur.h.
Data Fields | |
int | ell |
The fixed value of ell. More... | |
WaveformDataPiece * | m0_real_data |
The real (ell, 0) mode data piece. More... | |
WaveformDataPiece * | m0_imag_data |
The imag (ell, 0) mode data piece. More... | |
WaveformDataPiece ** | X_real_plus_data |
One Re[X_+] for each 1 <= m <= ell. More... | |
WaveformDataPiece ** | X_real_minus_data |
One Re[X_-] for each 1 <= m <= ell. More... | |
WaveformDataPiece ** | X_imag_plus_data |
One Im[X_+] for each 1 <= m <= ell. More... | |
WaveformDataPiece ** | X_imag_minus_data |
One Im[X_-] for each 1 <= m <= ell. More... | |
int WaveformFixedEllModeData::ell |
The fixed value of ell.
Definition at line 150 of file LALSimIMRPrecessingNRSur.h.
WaveformDataPiece* WaveformFixedEllModeData::m0_real_data |
The real (ell, 0) mode data piece.
Definition at line 151 of file LALSimIMRPrecessingNRSur.h.
WaveformDataPiece* WaveformFixedEllModeData::m0_imag_data |
The imag (ell, 0) mode data piece.
Definition at line 152 of file LALSimIMRPrecessingNRSur.h.
WaveformDataPiece** WaveformFixedEllModeData::X_real_plus_data |
One Re[X_+] for each 1 <= m <= ell.
Definition at line 153 of file LALSimIMRPrecessingNRSur.h.
WaveformDataPiece** WaveformFixedEllModeData::X_real_minus_data |
One Re[X_-] for each 1 <= m <= ell.
Definition at line 154 of file LALSimIMRPrecessingNRSur.h.
WaveformDataPiece** WaveformFixedEllModeData::X_imag_plus_data |
One Im[X_+] for each 1 <= m <= ell.
Definition at line 155 of file LALSimIMRPrecessingNRSur.h.
WaveformDataPiece** WaveformFixedEllModeData::X_imag_minus_data |
One Im[X_-] for each 1 <= m <= ell.
Definition at line 156 of file LALSimIMRPrecessingNRSur.h.