Utility functions for IMRPhenomX framework, arXiv:2001.11412. More...
Prototypes | |
REAL8 | XLALSimIMRPhenomXfMECO (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
Phenomenological fit to hybrid minimum energy circular orbit (MECO) function. More... | |
REAL8 | XLALSimIMRPhenomXfISCO (REAL8 chif) |
Fitting function for hybrid minimum energy circular orbit (MECO) function. More... | |
REAL8 | XLALSimIMRPhenomXErad2017 (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
Energy Radiated: X Jimenez-Forteza et al, PRD, 95, 064024, (2017), arXiv:1611.00332. More... | |
REAL8 | XLALSimIMRPhenomXFinalMass2017 (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
Final Mass = 1 - Energy Radiated, X Jimenez-Forteza et al, PRD, 95, 064024, (2017), arXiv:1611.00332. More... | |
REAL8 | XLALSimIMRPhenomXFinalSpin2017 (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
Final Dimensionless Spin, X Jimenez-Forteza et al, PRD, 95, 064024, (2017), arXiv:1611.00332. More... | |
REAL8 | XLALSimIMRPhenomXPrecessingFinalSpin2017 (const REAL8 eta, const REAL8 chi1L, const REAL8 chi2L, const REAL8 chi_inplane) |
Wrapper for the final spin in generically precessing binary black holes. More... | |
REAL8 | XLALSimIMRPhenomXchiPN (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
PN reduced spin parameter. More... | |
REAL8 | XLALSimIMRPhenomXchiPNHat (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
Normalised PN reduced spin parameter. More... | |
REAL8 | XLALSimIMRPhenomXchiEff (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
Effective aligned spin parameter. More... | |
REAL8 | XLALSimIMRPhenomXSTotR (REAL8 eta, REAL8 chi1L, REAL8 chi2L) |
Total spin normalised to [-1,1]. More... | |
REAL8 | XLALSimIMRPhenomXdchi (REAL8 chi1L, REAL8 chi2L) |
Spin difference. More... | |
REAL8 | XLALSimIMRPhenomXUtilsMftoHz (REAL8 Mf, REAL8 Mtot_Msun) |
Convert from geometric frequency to Hz. More... | |
REAL8 | XLALSimIMRPhenomXUtilsHztoMf (REAL8 fHz, REAL8 Mtot_Msun) |
Convert from frequency in Hz to geometric frequency. More... | |
REAL8 | XLALSimIMRPhenomXLina (REAL8 eta, REAL8 S, REAL8 dchi, REAL8 delta) |
We apply a linear time and phase shift to ~ align peak LinShift = (PNLina[ \(\eta,\chi_1,\chi_2\)] + \(\pi\) + f PNLinb[ \(\eta,\chi_1,\chi_2\)]); Linear time and phase shift: a + b*f. More... | |
REAL8 | XLALSimIMRPhenomXPsi4ToStrain (double eta, double S, double dchi) |
This is a fit of the time-difference between t_peak of strain and t_peak of psi4 needed to align in time our waveforms, which are calibrated to psi4. More... | |
REAL8 | XLALSimIMRPhenomXLinb (REAL8 eta, REAL8 S, REAL8 dchi, REAL8 delta) |
bool | IMRPhenomX_ApproxEqual (REAL8 x, REAL8 y, REAL8 epsilon) |
This function determines whether x and y are approximately equal to a relative accuracy epsilon. More... | |
void | IMRPhenomX_InternalNudge (REAL8 x, REAL8 X, REAL8 epsilon) |
If x and X are approximately equal to relative accuracy epsilon then set x = X. More... | |
REAL8 | XLALSimIMRPhenomXatan2tol (REAL8 a, REAL8 b, REAL8 tol) |
size_t | NextPow2 (const size_t n) |
bool | IMRPhenomX_StepFuncBool (const double t, const double t1) |
REAL8 | XLALSimIMRPhenomXsign (REAL8 x) |
double | pow_2_of (double number) |
calc square of number without floating point 'pow' More... | |
double | pow_3_of (double number) |
calc cube of number without floating point 'pow' More... | |
double | pow_4_of (double number) |
calc fourth power of number without floating point 'pow' More... | |
double | pow_5_of (double number) |
calc fifth power of number without floating point 'pow' More... | |
double | pow_6_of (double number) |
calc sixth power of number without floating point 'pow' More... | |
double | pow_7_of (double number) |
calc seventh power of number without floating point 'pow' More... | |
double | pow_8_of (double number) |
calc eigth power of number without floating point 'pow' More... | |
double | pow_9_of (double number) |
calc ninth power of number without floating point 'pow' More... | |
INT4 | XLALIMRPhenomXPCheckMassesAndSpins (REAL8 *m1, REAL8 *m2, REAL8 *chi1x, REAL8 *chi1y, REAL8 *chi1z, REAL8 *chi2x, REAL8 *chi2y, REAL8 *chi2z) |
Check if m1 > m2. More... | |
REAL8 | XLALSimIMRPhenomXRingdownPhase22AnsatzAnalytical (REAL8 ff, REAL8 fRD, REAL8 fDA, REAL8 a0, REAL8 a1, REAL8 a2, REAL8 a4, REAL8 aL) |
"Analytical" phenomenological ringdown ansatz for phase. More... | |
REAL8 | XLALSimIMRPhenomXRingdownPhaseDeriv22AnsatzAnalytical (REAL8 ff, REAL8 fRD, REAL8 fDA, REAL8 a0, REAL8 a1, REAL8 a2, REAL8 a4, REAL8 aL) |
"Analytical" phenomenological ringdown ansatz for phase derivative. More... | |
REAL8 | XLALSimIMRPhenomXRingdownAmplitude22AnsatzAnalytical (REAL8 ff, REAL8 fRD, REAL8 fDA, REAL8 gamma1, REAL8 gamma2, REAL8 gamma3) |
"Analytical" phenomenological ringdown ansatz for amplitude. More... | |
REAL8 | XLALSimIMRPhenomXIntermediateAmplitude22AnsatzAnalytical (REAL8 ff, REAL8 ff7o6, REAL8 a0, REAL8 a1, REAL8 a2, REAL8 a3, REAL8 a4, REAL8 a5) |
REAL8 | XLALSimIMRPhenomXIntermediatePhase22AnsatzAnalytical (REAL8 ff, REAL8 fRD, REAL8 fDA, REAL8 a0, REAL8 a1, REAL8 a2, REAL8 a3, REAL8 a4, REAL8 aL) |
REAL8 | XLALSimIMRPhenomXAmp22Prefactor (REAL8 eta) |
REAL8 | XLALSimIMRPhenomXfring22 (const REAL8 af) |
Ringdown frequency for 22 mode, given final dimensionless spin. More... | |
REAL8 | XLALSimIMRPhenomXfdamp22 (const REAL8 af) |
Damping frequency for 22 mode, given final dimensionless spin. More... | |
void | XLALSimIMRPhenomXUnwrapArray (double *in, double *out, int len) |
Function to unwrap a time series that contains an angle, to obtain a continuous time series. More... | |
Utility functions for IMRPhenomX framework, arXiv:2001.11412.
Definition in file LALSimIMRPhenomXUtilities.c.
Go to the source code of this file.
Phenomenological fit to hybrid minimum energy circular orbit (MECO) function.
Uses 3.5PN hybridised with test-particle limit. Reference: M Cabero et al, PRD, 95, 064016, (2017), arXiv:1602.03134
Definition at line 44 of file LALSimIMRPhenomXUtilities.c.
Fitting function for hybrid minimum energy circular orbit (MECO) function.
Definition at line 75 of file LALSimIMRPhenomXUtilities.c.
Energy Radiated: X Jimenez-Forteza et al, PRD, 95, 064024, (2017), arXiv:1611.00332.
Definition at line 104 of file LALSimIMRPhenomXUtilities.c.
Final Mass = 1 - Energy Radiated, X Jimenez-Forteza et al, PRD, 95, 064024, (2017), arXiv:1611.00332.
Definition at line 144 of file LALSimIMRPhenomXUtilities.c.
Final Dimensionless Spin, X Jimenez-Forteza et al, PRD, 95, 064024, (2017), arXiv:1611.00332.
Definition at line 185 of file LALSimIMRPhenomXUtilities.c.
REAL8 XLALSimIMRPhenomXPrecessingFinalSpin2017 | ( | const REAL8 | eta, |
const REAL8 | chi1L, | ||
const REAL8 | chi2L, | ||
const REAL8 | chi_inplane | ||
) |
Wrapper for the final spin in generically precessing binary black holes.
eta | Symmetric mass ratio |
chi1L | Aligned spin of BH 1 |
chi2L | Aligned spin of BH 2 |
chi_inplane | Effective precessions spin parameter, see Section IV D of arXiv:XXXX.YYYY |
Definition at line 225 of file LALSimIMRPhenomXUtilities.c.
PN reduced spin parameter.
Definition at line 257 of file LALSimIMRPhenomXUtilities.c.
Normalised PN reduced spin parameter.
Definition at line 270 of file LALSimIMRPhenomXUtilities.c.
Effective aligned spin parameter.
Definition at line 283 of file LALSimIMRPhenomXUtilities.c.
Total spin normalised to [-1,1].
Definition at line 295 of file LALSimIMRPhenomXUtilities.c.
Spin difference.
Definition at line 309 of file LALSimIMRPhenomXUtilities.c.
Convert from geometric frequency to Hz.
Mf | Geometric frequency |
Mtot_Msun | Total mass in solar masses |
Definition at line 318 of file LALSimIMRPhenomXUtilities.c.
Convert from frequency in Hz to geometric frequency.
fHz | Frequency in Hz |
Mtot_Msun | Total mass in solar masses |
Definition at line 329 of file LALSimIMRPhenomXUtilities.c.
We apply a linear time and phase shift to ~ align peak LinShift = (PNLina[ \(\eta,\chi_1,\chi_2\)] + \(\pi\) + f PNLinb[ \(\eta,\chi_1,\chi_2\)]); Linear time and phase shift: a + b*f.
eta | Geometric frequency |
S | Total mass in solar masses |
dchi | Total mass in solar masses |
delta | Total mass in solar masses |
Definition at line 342 of file LALSimIMRPhenomXUtilities.c.
REAL8 XLALSimIMRPhenomXPsi4ToStrain | ( | double | eta, |
double | S, | ||
double | dchi | ||
) |
This is a fit of the time-difference between t_peak of strain and t_peak of psi4 needed to align in time our waveforms, which are calibrated to psi4.
Definition at line 379 of file LALSimIMRPhenomXUtilities.c.
eta | Geometric frequency |
S | Total mass in solar masses |
dchi | Total mass in solar masses |
delta | Total mass in solar masses |
Definition at line 396 of file LALSimIMRPhenomXUtilities.c.
This function determines whether x and y are approximately equal to a relative accuracy epsilon.
Note that x and y are compared to relative accuracy, so this function is not suitable for testing whether a value is approximately zero.
Definition at line 423 of file LALSimIMRPhenomXUtilities.c.
If x and X are approximately equal to relative accuracy epsilon then set x = X.
If X = 0 then use an absolute comparison.
Definition at line 431 of file LALSimIMRPhenomXUtilities.c.
Definition at line 444 of file LALSimIMRPhenomXUtilities.c.
static size_t NextPow2 | ( | const size_t | n | ) |
Definition at line 455 of file LALSimIMRPhenomXUtilities.c.
bool IMRPhenomX_StepFuncBool | ( | const double | t, |
const double | t1 | ||
) |
Definition at line 461 of file LALSimIMRPhenomXUtilities.c.
Definition at line 465 of file LALSimIMRPhenomXUtilities.c.
double pow_2_of | ( | double | number | ) |
calc square of number without floating point 'pow'
Definition at line 475 of file LALSimIMRPhenomXUtilities.c.
double pow_3_of | ( | double | number | ) |
calc cube of number without floating point 'pow'
Definition at line 483 of file LALSimIMRPhenomXUtilities.c.
double pow_4_of | ( | double | number | ) |
calc fourth power of number without floating point 'pow'
Definition at line 491 of file LALSimIMRPhenomXUtilities.c.
double pow_5_of | ( | double | number | ) |
calc fifth power of number without floating point 'pow'
Definition at line 500 of file LALSimIMRPhenomXUtilities.c.
double pow_6_of | ( | double | number | ) |
calc sixth power of number without floating point 'pow'
Definition at line 509 of file LALSimIMRPhenomXUtilities.c.
double pow_7_of | ( | double | number | ) |
calc seventh power of number without floating point 'pow'
Definition at line 518 of file LALSimIMRPhenomXUtilities.c.
double pow_8_of | ( | double | number | ) |
calc eigth power of number without floating point 'pow'
Definition at line 527 of file LALSimIMRPhenomXUtilities.c.
double pow_9_of | ( | double | number | ) |
calc ninth power of number without floating point 'pow'
Definition at line 537 of file LALSimIMRPhenomXUtilities.c.
INT4 XLALIMRPhenomXPCheckMassesAndSpins | ( | REAL8 * | m1, |
REAL8 * | m2, | ||
REAL8 * | chi1x, | ||
REAL8 * | chi1y, | ||
REAL8 * | chi1z, | ||
REAL8 * | chi2x, | ||
REAL8 * | chi2y, | ||
REAL8 * | chi2z | ||
) |
Check if m1 > m2.
If not, swap the masses and spin vectors such that body is the heavier compact object.
[out] | m1 | mass of body 1 |
[out] | m2 | mass of body 2 |
[out] | chi1x | x-component of the dimensionless spin of object 1 w.r.t. Lhat = (0,0,1) |
[out] | chi1y | y-component of the dimensionless spin of object 1 w.r.t. Lhat = (0,0,1) |
[out] | chi1z | z-component of the dimensionless spin of object 1 w.r.t. Lhat = (0,0,1) |
[out] | chi2x | x-component of the dimensionless spin of object 2 w.r.t. Lhat = (0,0,1) |
[out] | chi2y | y-component of the dimensionless spin of object 2 w.r.t. Lhat = (0,0,1) |
[out] | chi2z | z-component of the dimensionless spin of object 2 w.r.t. Lhat = (0,0,1) |
Definition at line 547 of file LALSimIMRPhenomXUtilities.c.
REAL8 XLALSimIMRPhenomXRingdownPhase22AnsatzAnalytical | ( | REAL8 | ff, |
REAL8 | fRD, | ||
REAL8 | fDA, | ||
REAL8 | a0, | ||
REAL8 | a1, | ||
REAL8 | a2, | ||
REAL8 | a4, | ||
REAL8 | aL | ||
) |
"Analytical" phenomenological ringdown ansatz for phase.
This is used by the higher mode functions and can be used to prototype or test model. Convenient wrapper exposed via XLAL.
Definition at line 619 of file LALSimIMRPhenomXUtilities.c.
REAL8 XLALSimIMRPhenomXRingdownPhaseDeriv22AnsatzAnalytical | ( | REAL8 | ff, |
REAL8 | fRD, | ||
REAL8 | fDA, | ||
REAL8 | a0, | ||
REAL8 | a1, | ||
REAL8 | a2, | ||
REAL8 | a4, | ||
REAL8 | aL | ||
) |
"Analytical" phenomenological ringdown ansatz for phase derivative.
This is used by the higher mode functions and can be used to prototype or test model. Convenient wrapper exposed via XLAL.
a_0 + a_1 f^(-1) + a_2 f^(-2) + a_3 f^(-3) + a_4 f^(-4) + ( aRD ) / ( (f_damp^2 + (f - f_ring)^2 ) )
where a_L = - dphase0 * aRD
Our canonical ringdown ansatz sets a_3 = 0.
Definition at line 645 of file LALSimIMRPhenomXUtilities.c.
REAL8 XLALSimIMRPhenomXRingdownAmplitude22AnsatzAnalytical | ( | REAL8 | ff, |
REAL8 | fRD, | ||
REAL8 | fDA, | ||
REAL8 | gamma1, | ||
REAL8 | gamma2, | ||
REAL8 | gamma3 | ||
) |
"Analytical" phenomenological ringdown ansatz for amplitude.
This is used by the higher mode functions but can also be used to prototype or test model. Convenient wrapper exposed via XLAL.
Definition at line 664 of file LALSimIMRPhenomXUtilities.c.
REAL8 XLALSimIMRPhenomXIntermediateAmplitude22AnsatzAnalytical | ( | REAL8 | ff, |
REAL8 | ff7o6, | ||
REAL8 | a0, | ||
REAL8 | a1, | ||
REAL8 | a2, | ||
REAL8 | a3, | ||
REAL8 | a4, | ||
REAL8 | a5 | ||
) |
Definition at line 684 of file LALSimIMRPhenomXUtilities.c.
REAL8 XLALSimIMRPhenomXIntermediatePhase22AnsatzAnalytical | ( | REAL8 | ff, |
REAL8 | fRD, | ||
REAL8 | fDA, | ||
REAL8 | a0, | ||
REAL8 | a1, | ||
REAL8 | a2, | ||
REAL8 | a3, | ||
REAL8 | a4, | ||
REAL8 | aL | ||
) |
Definition at line 696 of file LALSimIMRPhenomXUtilities.c.
Definition at line 716 of file LALSimIMRPhenomXUtilities.c.
Ringdown frequency for 22 mode, given final dimensionless spin.
https://arxiv.org/src/2001.10914v1/anc/QNMs/CoefficientStatsfring22.m
Definition at line 735 of file LALSimIMRPhenomXUtilities.c.
Damping frequency for 22 mode, given final dimensionless spin.
https://arxiv.org/src/2001.10914v1/anc/QNMs/CoefficientStatsfdamp22.m
Definition at line 769 of file LALSimIMRPhenomXUtilities.c.
void XLALSimIMRPhenomXUnwrapArray | ( | double * | in, |
double * | out, | ||
int | len | ||
) |
Function to unwrap a time series that contains an angle, to obtain a continuous time series.
Definition at line 796 of file LALSimIMRPhenomXUtilities.c.