コード例 #1
0
 def getswigrow(self, glue_row):
     """Translates glue row from the table to libmetaio row"""
     import lalmetaio as lmt
     swigrow = lmt.SimInspiralTable()
     for simattr in lsctables.SimInspiralTable.validcolumns.keys():
         if simattr in ["waveform", "source", "numrel_data", "taper"]:
             setattr(swigrow, simattr, str(getattr(glue_row, simattr)))
         else:
             setattr(swigrow, simattr, getattr(glue_row, simattr))
     swigrow.geocent_end_time.gpsNanoSeconds = glue_row.geocent_end_time_ns
     return swigrow
コード例 #2
0
def get_eff_dist(detector, ra, dec, inclination, polarization, epoch, gmst):
    sim_inspiral = lalmetaio.SimInspiralTable()
    sim_inspiral.distance = 1
    sim_inspiral.longitude = ra
    sim_inspiral.latitude = dec
    sim_inspiral.inclination = inclination
    sim_inspiral.polarization = polarization
    sim_inspiral.geocent_end_time = epoch
    sim_inspiral.end_time_gmst = gmst
    _ = lal.LIGOTimeGPS()
    _, eff_dist = lalinspiral.InspiralSiteTimeAndDist(sim_inspiral, detector,
                                                      _)
    return eff_dist
コード例 #3
0
def _get_waveform_from_inspiral(**p):
    import lalmetaio

    # prefix with 'Inspiral-'
    name = p['approximant'][9:]

    if name.startswith('EOB'):
        p['phase_order'] = -8

    params = lalmetaio.SimInspiralTable()
    params.waveform = name + string_from_order[p['phase_order']]
    params.mass1 = p['mass1']
    params.mass2 = p['mass2']
    params.f_lower = p['f_lower']
    params.spin1x = p['spin1x']
    params.spin1y = p['spin1y']
    params.spin1z = p['spin1z']
    params.spin2x = p['spin2x']
    params.spin2y = p['spin2y']
    params.spin2z = p['spin2z']
    params.inclination = p['inclination']
    params.distance = p['distance']
    params.coa_phase = p['coa_phase']

    guess_length = lalinspiral.FindChirpChirpTime(params.mass1, params.mass2,
                                                  params.f_lower, 7)
    guess_length = max(guess_length, 3)
    params.geocent_end_time = guess_length * 1.5
    params.taper = 'TAPER_NONE'  #FIXME - either explain or don't hardcode this
    bufferl = guess_length * 2
    dt = p['delta_t']
    df = 1.0 / bufferl
    sample_rate = int(1.0 / dt)
    epoch = lal.LIGOTimeGPS(0, 0)
    N = bufferl * sample_rate
    n = N / 2 + 1

    resp = FrequencySeries(zeros(n), delta_f=df, epoch=epoch,
                           dtype=complex64) + 1
    out = TimeSeries(zeros(N), delta_t=dt, epoch=epoch, dtype=float32)
    outl = out.lal()
    outl.sampleUnits = lal.ADCCountUnit

    out2 = TimeSeries(zeros(N), delta_t=dt, epoch=epoch, dtype=float32)
    outl2 = out.lal()
    outl2.sampleUnits = lal.ADCCountUnit

    respl = resp.lal()
    respl.sampleUnits = lal.DimensionlessUnit

    lalinspiral.FindChirpInjectSignals(outl, params, respl)

    params.coa_phase -= lal.PI / 4
    lalinspiral.FindChirpInjectSignals(outl2, params, respl)
    seriesp = TimeSeries(outl.data.data,
                         delta_t=dt,
                         epoch=epoch - params.geocent_end_time)

    seriesc = TimeSeries(outl2.data.data,
                         delta_t=dt,
                         epoch=epoch - params.geocent_end_time)

    return seriesp, seriesc