예제 #1
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def print_fd_approximants():
    """Only list the frequency-domain approximants in lalsimulation.
    """
    napprox = lalsimulation.NumApproximants
    for i in range(napprox):
        if lalsimulation.SimInspiralImplementedFDApproximants(i):
            print i, lalsimulation.GetStringFromApproximant(i)
예제 #2
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    def _compute_waveform_comps(self, df, f_final):
        approx = lalsim.GetApproximantFromString(self.approximant)
        lmbda1 = lmbda2 = 0  # No tidal terms here
        ampO = -1  # Are these the correct values??
        phaseO = -1  # Are these the correct values??

        if lalsim.SimInspiralImplementedFDApproximants(approx):
            hplus_fd, hcross_fd = lalsim.SimInspiralChooseFDWaveform(
                self.orb_phase,
                df,
                self.m1 * MSUN_SI,
                self.m2 * MSUN_SI,
                self.spin1x,
                self.spin1y,
                self.spin1z,
                self.spin2x,
                self.spin2y,
                self.spin2z,
                self.bank.flow,
                f_final,
                self.bank.flow,
                1e6 * PC_SI,
                self.iota,
                lmbda1,
                lmbda2,  # irrelevant parameters for BBH
                None,
                None,  # non-GR parameters
                ampO,
                phaseO,
                approx)
        else:
            hplus_fd, hcross_fd = lalsim.SimInspiralFD(
                self.orb_phase,
                df,
                self.m1 * MSUN_SI,
                self.m2 * MSUN_SI,
                self.spin1x,
                self.spin1y,
                self.spin1z,
                self.spin2x,
                self.spin2y,
                self.spin2z,
                self.bank.flow,
                f_final,
                self.bank.flow,
                1e6 * PC_SI,
                0,
                self.iota,
                lmbda1,
                lmbda2,  # irrelevant parameters for BBH
                None,
                None,  # non-GR parameters
                ampO,
                phaseO,
                approx)

        return hplus_fd, hcross_fd
예제 #3
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    def _compute_waveform_comps(self, df, f_final):
        approx = lalsim.GetApproximantFromString(self.approximant)
        if lalsim.SimInspiralImplementedFDApproximants(approx):
            hplus_fd, hcross_fd = lalsim.SimInspiralChooseFDWaveform(
                self.m1 * MSUN_SI, self.m2 * MSUN_SI, self.spin1x, self.spin1y,
                self.spin1z, self.spin2x, self.spin2y, self.spin2z,
                1.e6 * PC_SI, self.iota, self.orb_phase, 0., 0., 0., df,
                self.flow, f_final, self.flow, None, approx)
        else:
            hplus_fd, hcross_fd = lalsim.SimInspiralFD(
                self.m1 * MSUN_SI, self.m2 * MSUN_SI, self.spin1x, self.spin1y,
                self.spin1z, self.spin2x, self.spin2y, self.spin2z,
                1.e6 * PC_SI, self.iota, self.orb_phase, 0., 0., 0., df,
                self.flow, f_final, self.flow, None, approx)

        return hplus_fd, hcross_fd
예제 #4
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    def _compute_waveform(self, df, f_final):

        approx = lalsim.GetApproximantFromString(self.approximant)

        if lalsim.SimInspiralImplementedFDApproximants(approx):
            hplus_fd, hcross_fd = lalsim.SimInspiralChooseFDWaveform(
                self.m1 * MSUN_SI, self.m2 * MSUN_SI, 0., 0., self.spin1z, 0.,
                0., self.spin2z, 1e6 * PC_SI, 0., 0., 0., 0., 0., df,
                self.bank.flow, f_final, self.bank.flow, None, approx)

        else:
            hplus_fd, hcross_fd = lalsim.SimInspiralFD(
                phi0, df, self.m1 * MSUN_SI, self.m2 * MSUN_SI, 0, 0,
                self.spin1z, 0, 0, self.spin2z, 1.e6 * PC_SI, 0., 0., 0., 0.,
                0., df, self.bank.flow, f_final, 40., None, approx)
        return hplus_fd
예제 #5
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파일: waveforms.py 프로젝트: spxiwh/sbank
    def _compute_waveform(self, df, f_final):

        phi0 = 0  # This is a reference phase, and not an intrinsic parameter
        approx = lalsim.GetApproximantFromString(self.approximant)

        if lalsim.SimInspiralImplementedFDApproximants(approx):
            hplus_fd, hcross_fd = lalsim.SimInspiralChooseFDWaveform(
                self.m1 * MSUN_SI, self.m2 * MSUN_SI, 0., 0., self.spin1z, 0.,
                0., self.spin2z, 1e6 * PC_SI, 0., 0., 0., 0., 0., df,
                self.flow, f_final, self.flow, None, approx)

        else:
            hplus_fd, hcross_fd = lalsim.SimInspiralFD(
                phi0, df, self.m1 * MSUN_SI, self.m2 * MSUN_SI, 0, 0,
                self.spin1z, 0, 0, self.spin2z, 1.e6 * PC_SI, 0., 0., 0., 0.,
                0., df, self.flow, f_final, 40., None, approx)
        return hplus_fd
예제 #6
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    def _compute_waveform(self, df, f_final):

        flags = lalsim.SimInspiralCreateWaveformFlags()
        phi0 = 0  # This is a reference phase, and not an intrinsic parameter
        lmbda1 = lmbda2 = 0  # No tidal terms here
        ampO = -1  # Are these the correct values??
        phaseO = -1  # Are these the correct values??
        approx = lalsim.GetApproximantFromString(self.approximant)

        if lalsim.SimInspiralImplementedFDApproximants(approx):
            hplus_fd, hcross_fd = lalsim.SimInspiralChooseFDWaveform(
                0, df, self.m1 * MSUN_SI, self.m2 * MSUN_SI, 0., 0.,
                self.spin1z, 0., 0., self.spin2z, self.bank.flow, f_final,
                self.bank.flow, 1e6 * PC_SI, 0., 0., 0., flags, None, ampO,
                phaseO, approx)

        else:
            hplus_fd, hcross_fd = lalsim.SimInspiralFD(
                phi0,
                df,
                self.m1 * MSUN_SI,
                self.m2 * MSUN_SI,
                0,
                0,
                self.spin1z,
                0,
                0,
                self.spin2z,
                self.bank.flow,
                f_final,
                40.0,
                1e6 * PC_SI,
                0,
                0,
                lmbda1,
                lmbda2,  # irrelevant parameters for BBH
                None,
                None,  # non-GR parameters
                ampO,
                phaseO,
                approx)

        return hplus_fd
예제 #7
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import pytest
import lalsimulation as lalsim

# Function to get the name of a function
def get_name(f):
    return f.__name__

# Set of functions to test
func_list = [
    lalsim.SimInspiralGetSpinSupportFromApproximant,
    lalsim.SimInspiralGetSpinFreqFromApproximant,
    lalsim.SimInspiralApproximantAcceptTestGRParams
]

# Loop over all implemented TD or FD approximants

IMPLEMENTED = [
    k for k in range(lalsim.NumApproximants) if
    lalsim.SimInspiralImplementedTDApproximants(k) or
    lalsim.SimInspiralImplementedFDApproximants(k)
]

@pytest.mark.parametrize("func", func_list, ids=get_name)
@pytest.mark.parametrize("k", IMPLEMENTED, ids=lalsim.GetStringFromApproximant)
def test_wf_property_lists(k, func):
    func(k)

if __name__ == '__main__':
    args = sys.argv[1:] or ["-v", "-rs", "--junit-xml=junit-wf_property_lists.xml"]
    sys.exit(pytest.main(args=[__file__] + args))
예제 #8
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               float(p['polarization']),
               float(p['delta_t']))

    hp = TimeSeries(hp.data.data[:], delta_t=hp.deltaT, epoch=hp.epoch)
    hc = TimeSeries(hc.data.data[:], delta_t=hc.deltaT, epoch=hc.epoch)

    return hp, hc

for approx_enum in xrange(0, lalsimulation.NumApproximants):
    if lalsimulation.SimInspiralImplementedTDApproximants(approx_enum):
        approx_name = lalsimulation.GetStringFromApproximant(approx_enum)
        _lalsim_enum[approx_name] = approx_enum
        _lalsim_td_approximants[approx_name] = _lalsim_td_waveform

for approx_enum in xrange(0, lalsimulation.NumApproximants):
    if lalsimulation.SimInspiralImplementedFDApproximants(approx_enum):
        approx_name = lalsimulation.GetStringFromApproximant(approx_enum)
        _lalsim_enum[approx_name] = approx_enum
        _lalsim_fd_approximants[approx_name] = _lalsim_fd_waveform

# sine-Gaussian burst
for approx_enum in xrange(0, lalsimulation.NumApproximants):
    if lalsimulation.SimInspiralImplementedFDApproximants(approx_enum):
        approx_name = lalsimulation.GetStringFromApproximant(approx_enum)
        _lalsim_enum[approx_name] = approx_enum
        _lalsim_sgburst_approximants[approx_name] = _lalsim_sgburst_waveform

cpu_sgburst = _lalsim_sgburst_approximants

cpu_td = dict(_lalsim_td_approximants.items())
cpu_fd = _lalsim_fd_approximants
예제 #9
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def _base_lal_cbc_fd_waveform(
        frequency_array, mass_1, mass_2, luminosity_distance, theta_jn, phase,
        a_1=0.0, a_2=0.0, tilt_1=0.0, tilt_2=0.0, phi_12=0.0, phi_jl=0.0,
        lambda_1=0.0, lambda_2=0.0, eccentricity=0.0, **waveform_kwargs):
    """ Generate a cbc waveform model using lalsimulation

    Parameters
    ==========
    frequency_array: array_like
        The frequencies at which we want to calculate the strain
    mass_1: float
        The mass of the heavier object in solar masses
    mass_2: float
        The mass of the lighter object in solar masses
    luminosity_distance: float
        The luminosity distance in megaparsec
    a_1: float
        Dimensionless primary spin magnitude
    tilt_1: float
        Primary tilt angle
    phi_12: float
        Azimuthal angle between the component spins
    a_2: float
        Dimensionless secondary spin magnitude
    tilt_2: float
        Secondary tilt angle
    phi_jl: float
        Azimuthal angle between the total and orbital angular momenta
    theta_jn: float
        Orbital inclination
    phase: float
        The phase at coalescence
    eccentricity: float
        Binary eccentricity
    lambda_1: float
        Tidal deformability of the more massive object
    lambda_2: float
        Tidal deformability of the less massive object
    kwargs: dict
        Optional keyword arguments

    Returns
    =======
    dict: A dictionary with the plus and cross polarisation strain modes
    """
    import lal
    import lalsimulation as lalsim

    waveform_approximant = waveform_kwargs['waveform_approximant']
    reference_frequency = waveform_kwargs['reference_frequency']
    minimum_frequency = waveform_kwargs['minimum_frequency']
    maximum_frequency = waveform_kwargs['maximum_frequency']
    catch_waveform_errors = waveform_kwargs['catch_waveform_errors']
    pn_spin_order = waveform_kwargs['pn_spin_order']
    pn_tidal_order = waveform_kwargs['pn_tidal_order']
    pn_phase_order = waveform_kwargs['pn_phase_order']
    pn_amplitude_order = waveform_kwargs['pn_amplitude_order']
    waveform_dictionary = waveform_kwargs.get(
        'lal_waveform_dictionary', lal.CreateDict()
    )

    approximant = lalsim_GetApproximantFromString(waveform_approximant)

    if pn_amplitude_order != 0:
        start_frequency = lalsim.SimInspiralfLow2fStart(
            minimum_frequency, int(pn_amplitude_order), approximant)
    else:
        start_frequency = minimum_frequency

    delta_frequency = frequency_array[1] - frequency_array[0]

    frequency_bounds = ((frequency_array >= minimum_frequency) *
                        (frequency_array <= maximum_frequency))

    luminosity_distance = luminosity_distance * 1e6 * utils.parsec
    mass_1 = mass_1 * utils.solar_mass
    mass_2 = mass_2 * utils.solar_mass

    iota, spin_1x, spin_1y, spin_1z, spin_2x, spin_2y, spin_2z = bilby_to_lalsimulation_spins(
        theta_jn=theta_jn, phi_jl=phi_jl, tilt_1=tilt_1, tilt_2=tilt_2,
        phi_12=phi_12, a_1=a_1, a_2=a_2, mass_1=mass_1, mass_2=mass_2,
        reference_frequency=reference_frequency, phase=phase)

    longitude_ascending_nodes = 0.0
    mean_per_ano = 0.0

    lalsim.SimInspiralWaveformParamsInsertPNSpinOrder(
        waveform_dictionary, int(pn_spin_order))
    lalsim.SimInspiralWaveformParamsInsertPNTidalOrder(
        waveform_dictionary, int(pn_tidal_order))
    lalsim.SimInspiralWaveformParamsInsertPNPhaseOrder(
        waveform_dictionary, int(pn_phase_order))
    lalsim.SimInspiralWaveformParamsInsertPNAmplitudeOrder(
        waveform_dictionary, int(pn_amplitude_order))
    lalsim_SimInspiralWaveformParamsInsertTidalLambda1(
        waveform_dictionary, lambda_1)
    lalsim_SimInspiralWaveformParamsInsertTidalLambda2(
        waveform_dictionary, lambda_2)

    for key, value in waveform_kwargs.items():
        func = getattr(lalsim, "SimInspiralWaveformParamsInsert" + key, None)
        if func is not None:
            func(waveform_dictionary, value)

    if waveform_kwargs.get('numerical_relativity_file', None) is not None:
        lalsim.SimInspiralWaveformParamsInsertNumRelData(
            waveform_dictionary, waveform_kwargs['numerical_relativity_file'])

    if ('mode_array' in waveform_kwargs) and waveform_kwargs['mode_array'] is not None:
        mode_array = waveform_kwargs['mode_array']
        mode_array_lal = lalsim.SimInspiralCreateModeArray()
        for mode in mode_array:
            lalsim.SimInspiralModeArrayActivateMode(mode_array_lal, mode[0], mode[1])
        lalsim.SimInspiralWaveformParamsInsertModeArray(waveform_dictionary, mode_array_lal)

    if lalsim.SimInspiralImplementedFDApproximants(approximant):
        wf_func = lalsim_SimInspiralChooseFDWaveform
    else:
        wf_func = lalsim_SimInspiralFD
    try:
        hplus, hcross = wf_func(
            mass_1, mass_2, spin_1x, spin_1y, spin_1z, spin_2x, spin_2y,
            spin_2z, luminosity_distance, iota, phase,
            longitude_ascending_nodes, eccentricity, mean_per_ano, delta_frequency,
            start_frequency, maximum_frequency, reference_frequency,
            waveform_dictionary, approximant)
    except Exception as e:
        if not catch_waveform_errors:
            raise
        else:
            EDOM = (e.args[0] == 'Internal function call failed: Input domain error')
            if EDOM:
                failed_parameters = dict(mass_1=mass_1, mass_2=mass_2,
                                         spin_1=(spin_1x, spin_2y, spin_1z),
                                         spin_2=(spin_2x, spin_2y, spin_2z),
                                         luminosity_distance=luminosity_distance,
                                         iota=iota, phase=phase,
                                         eccentricity=eccentricity,
                                         start_frequency=start_frequency)
                logger.warning("Evaluating the waveform failed with error: {}\n".format(e) +
                               "The parameters were {}\n".format(failed_parameters) +
                               "Likelihood will be set to -inf.")
                return None
            else:
                raise

    h_plus = np.zeros_like(frequency_array, dtype=complex)
    h_cross = np.zeros_like(frequency_array, dtype=complex)

    if len(hplus.data.data) > len(frequency_array):
        logger.debug("LALsim waveform longer than bilby's `frequency_array`" +
                     "({} vs {}), ".format(len(hplus.data.data), len(frequency_array)) +
                     "probably because padded with zeros up to the next power of two length." +
                     " Truncating lalsim array.")
        h_plus = hplus.data.data[:len(h_plus)]
        h_cross = hcross.data.data[:len(h_cross)]
    else:
        h_plus[:len(hplus.data.data)] = hplus.data.data
        h_cross[:len(hcross.data.data)] = hcross.data.data

    h_plus *= frequency_bounds
    h_cross *= frequency_bounds

    if wf_func == lalsim_SimInspiralFD:
        dt = 1 / hplus.deltaF + (hplus.epoch.gpsSeconds + hplus.epoch.gpsNanoSeconds * 1e-9)
        time_shift = np.exp(-1j * 2 * np.pi * dt * frequency_array[frequency_bounds])
        h_plus[frequency_bounds] *= time_shift
        h_cross[frequency_bounds] *= time_shift

    return dict(plus=h_plus, cross=h_cross)
예제 #10
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    base_dir =''  # all directories are provided as full path names


if opts.choose_data_LI_seglen:
    cmd_event = "gracedb_legacy download " + opts.gracedb_id + " coinc.xml"
    os.system(cmd_event)
    event_dict = retrieve_event_from_coinc("coinc.xml")
    P=lalsimutils.ChooseWaveformParams()
    P.m1 = event_dict["m1"]*lal.MSUN_SI; P.m2=event_dict["m2"]*lal.MSUN_SI; P.s1z = event_dict["s1z"]; P.s2z = event_dict["s2z"]
    P.fmin = opts.fmin  #  fmin we will use internally
    T_wave = lalsimutils.estimateWaveformDuration(P) +2  # 2 second buffer on end; note that with next power of 2, will go up to 4s
    T_wave_round = lalsimutils.nextPow2( T_wave)

    # For frequency-domain approximants, I need another factor of 2!
    # We have an extra buffer
    if lalsim.SimInspiralImplementedFDApproximants(P.approx)==1:
            print( " FD approximant, needs extra buffer for RIFT at present ")
            T_wave_round *=2 

    print( " Assigning auto-selected segment length ", T_wave_round)
    opts.data_LI_seglen  = T_wave_round

    # Problem with SEOBNRv3 starting frequencies
    mtot_msun = event_dict["m1"]+event_dict["m2"] 
    if ('SEOB' in opts.approx) and mtot_msun > 90*(20./opts.fmin):
            fmin_template = int(14*(90/mtot_msun))   # should also decrease this due to lmax!
            print( "  SEOB starting frequencies need to be reduced for this event; trying ", fmin_template)


is_analysis_precessing =False
if opts.approx == "SEOBNRv3" or opts.approx == "NRSur7dq2" or opts.approx == "NRSur7dq4" or (opts.approx == 'SEOBNv3_opt') or (opts.approx == 'IMRPhenomPv2') or (opts.approx =="SEOBNRv4P" ) or (opts.approx == "SEOBNRv4PHM") or ('SpinTaylor' in opts.approx):
예제 #11
0
파일: source.py 프로젝트: yi-fan-wang/bilby
def _base_lal_cbc_fd_waveform(frequency_array,
                              mass_1,
                              mass_2,
                              luminosity_distance,
                              theta_jn,
                              phase,
                              a_1=0.0,
                              a_2=0.0,
                              tilt_1=0.0,
                              tilt_2=0.0,
                              phi_12=0.0,
                              phi_jl=0.0,
                              lambda_1=0.0,
                              lambda_2=0.0,
                              eccentricity=0.0,
                              **waveform_kwargs):
    """ Generate a cbc waveform model using lalsimulation

    Parameters
    ----------
    frequency_array: array_like
        The frequencies at which we want to calculate the strain
    mass_1: float
        The mass of the heavier object in solar masses
    mass_2: float
        The mass of the lighter object in solar masses
    luminosity_distance: float
        The luminosity distance in megaparsec
    a_1: float
        Dimensionless primary spin magnitude
    tilt_1: float
        Primary tilt angle
    phi_12: float
        Azimuthal angle between the component spins
    a_2: float
        Dimensionless secondary spin magnitude
    tilt_2: float
        Secondary tilt angle
    phi_jl: float
        Azimuthal angle between the total and orbital angular momenta
    theta_jn: float
        Orbital inclination
    phase: float
        The phase at coalescence
    eccentricity: float
        Binary eccentricity
    lambda_1: float
        Tidal deformability of the more massive object
    lambda_2: float
        Tidal deformability of the less massive object
    kwargs: dict
        Optional keyword arguments

    Returns
    -------
    dict: A dictionary with the plus and cross polarisation strain modes
    """
    waveform_approximant = waveform_kwargs['waveform_approximant']
    reference_frequency = waveform_kwargs['reference_frequency']
    minimum_frequency = waveform_kwargs['minimum_frequency']
    maximum_frequency = waveform_kwargs['maximum_frequency']
    catch_waveform_errors = waveform_kwargs['catch_waveform_errors']
    pn_spin_order = waveform_kwargs['pn_spin_order']
    pn_tidal_order = waveform_kwargs['pn_tidal_order']
    pn_phase_order = waveform_kwargs['pn_phase_order']
    pn_amplitude_order = waveform_kwargs['pn_amplitude_order']

    approximant = lalsim_GetApproximantFromString(waveform_approximant)

    if pn_amplitude_order != 0:
        start_frequency = lalsim.SimInspiralfLow2fStart(
            minimum_frequency, int(pn_amplitude_order), approximant)
    else:
        start_frequency = minimum_frequency

    delta_frequency = frequency_array[1] - frequency_array[0]

    frequency_bounds = ((frequency_array >= minimum_frequency) *
                        (frequency_array <= maximum_frequency))

    luminosity_distance = luminosity_distance * 1e6 * utils.parsec
    mass_1 = mass_1 * utils.solar_mass
    mass_2 = mass_2 * utils.solar_mass

    iota, spin_1x, spin_1y, spin_1z, spin_2x, spin_2y, spin_2z = bilby_to_lalsimulation_spins(
        theta_jn=theta_jn,
        phi_jl=phi_jl,
        tilt_1=tilt_1,
        tilt_2=tilt_2,
        phi_12=phi_12,
        a_1=a_1,
        a_2=a_2,
        mass_1=mass_1,
        mass_2=mass_2,
        reference_frequency=reference_frequency,
        phase=phase)

    longitude_ascending_nodes = 0.0
    mean_per_ano = 0.0

    waveform_dictionary = lal.CreateDict()
    lalsim.SimInspiralWaveformParamsInsertPNSpinOrder(waveform_dictionary,
                                                      int(pn_spin_order))
    lalsim.SimInspiralWaveformParamsInsertPNTidalOrder(waveform_dictionary,
                                                       int(pn_tidal_order))
    lalsim.SimInspiralWaveformParamsInsertPNPhaseOrder(waveform_dictionary,
                                                       int(pn_phase_order))
    lalsim.SimInspiralWaveformParamsInsertPNAmplitudeOrder(
        waveform_dictionary, int(pn_amplitude_order))
    lalsim_SimInspiralWaveformParamsInsertTidalLambda1(waveform_dictionary,
                                                       lambda_1)
    lalsim_SimInspiralWaveformParamsInsertTidalLambda2(waveform_dictionary,
                                                       lambda_2)

    if 'modearray' in waveform_kwargs:
        modearray = waveform_kwargs['modearray']
        mode_array = lalsim.SimInspiralCreateModeArray()
        for mode in modearray:
            lalsim.SimInspiralModeArrayActivateMode(mode_array, mode[0],
                                                    mode[1])
        lalsim.SimInspiralWaveformParamsInsertModeArray(
            waveform_dictionary, mode_array)

    if lalsim.SimInspiralImplementedFDApproximants(approximant):
        wf_func = lalsim_SimInspiralChooseFDWaveform
    else:
        wf_func = lalsim_SimInspiralFD
    try:
        hplus, hcross = wf_func(mass_1, mass_2, spin_1x, spin_1y, spin_1z,
                                spin_2x, spin_2y, spin_2z, luminosity_distance,
                                iota, phase, longitude_ascending_nodes,
                                eccentricity, mean_per_ano, delta_frequency,
                                start_frequency, maximum_frequency,
                                reference_frequency, waveform_dictionary,
                                approximant)
    except Exception as e:
        if not catch_waveform_errors:
            raise
        else:
            EDOM = (e.args[0] ==
                    'Internal function call failed: Input domain error')
            if EDOM:
                failed_parameters = dict(
                    mass_1=mass_1,
                    mass_2=mass_2,
                    spin_1=(spin_1x, spin_2y, spin_1z),
                    spin_2=(spin_2x, spin_2y, spin_2z),
                    luminosity_distance=luminosity_distance,
                    iota=iota,
                    phase=phase,
                    eccentricity=eccentricity,
                    start_frequency=start_frequency)
                logger.warning(
                    "Evaluating the waveform failed with error: {}\n".format(e)
                    + "The parameters were {}\n".format(failed_parameters) +
                    "Likelihood will be set to -inf.")
                return None
            else:
                raise

    h_plus = np.zeros_like(frequency_array, dtype=np.complex)
    h_cross = np.zeros_like(frequency_array, dtype=np.complex)

    if len(hplus.data.data) > len(frequency_array):
        raise ValueError("Waveform longer than frequency array")

    h_plus[:len(hplus.data.data)] = hplus.data.data
    h_cross[:len(hcross.data.data)] = hcross.data.data

    h_plus *= frequency_bounds
    h_cross *= frequency_bounds

    return dict(plus=h_plus, cross=h_cross)