Skip to content
Snippets Groups Projects
Commit f7311ed6 authored by Gregory Ashton's avatar Gregory Ashton
Browse files

Merge branch 'develop-GA' of gitlab.aei.uni-hannover.de:GregAshton/PyFstat into develop-GA

parents adb2e3d2 f93e27b1
No related branches found
No related tags found
No related merge requests found
Showing
with 301 additions and 245 deletions
test_app:
script:
- . /home/greg/lalsuite-install/etc/lalapps-user-env.sh
- /home/greg/anaconda2/bin/python tests.py TestWriter
- /home/greg/anaconda2/bin/python tests.py TestBaseSearchClass
- /home/greg/anaconda2/bin/python tests.py TestComputeFstat
- /home/greg/anaconda2/bin/python tests.py TestSemiCoherentGlitchSearch
- /home/greg/anaconda2/bin/python tests.py Writer
- /home/greg/anaconda2/bin/python tests.py par
- /home/greg/anaconda2/bin/python tests.py BaseSearchClass
- /home/greg/anaconda2/bin/python tests.py ComputeFstat
- /home/greg/anaconda2/bin/python tests.py SemiCoherentSearch
- /home/greg/anaconda2/bin/python tests.py SemiCoherentGlitchSearch
- /home/greg/anaconda2/bin/python tests.py MCMCSearch
- /home/greg/anaconda2/bin/python tests.py GridSearch
......@@ -47,8 +47,8 @@ theta_prior = {'F0': {'type': 'unif',
'Delta': Delta
}
ntemps = 1
log10beta_min = -1
ntemps = 2
log10beta_min = -0.5
nwalkers = 100
nsteps = [300, 300]
......@@ -57,6 +57,9 @@ mcmc = pyfstat.MCMCSearch(
sftfilepattern='{}/*{}*sft'.format(outdir, label), theta_prior=theta_prior,
tref=tref, minStartTime=tstart, maxStartTime=tend, nsteps=nsteps,
nwalkers=nwalkers, ntemps=ntemps, log10beta_min=log10beta_min)
mcmc.run(subtractions=[F0, F1])
mcmc.transform_dictionary = dict(
F0=dict(subtractor=F0, symbol='$f-f^\mathrm{s}$'),
F1=dict(subtractor=F1, symbol='$\dot{f}-\dot{f}^\mathrm{s}$'))
mcmc.run()
mcmc.plot_corner(add_prior=True)
mcmc.print_summary()
import numpy as np
from pyfstat import MCMCSearch
F0 = 30.0
F1 = -1e-10
F2 = 0
Alpha = np.radians(83.6292)
Delta = np.radians(22.0144)
tref = 362750407.0
tstart = 1000000000
duration = 100*86400
tend = tstart + duration
theta_prior = {'F0': {'type': 'unif', 'lower': F0-1e-4, 'upper': F0+1e-4},
'F1': {'type': 'unif', 'lower': F1*(1+1e-3), 'upper': F1*(1-1e-3)},
'F2': F2,
'Alpha': Alpha,
'Delta': Delta
}
ntemps = 2
log10beta_min = -0.01
nwalkers = 100
nsteps = [500, 500]
mcmc = MCMCSearch('fully_coherent_search_using_MCMC_on_glitching_data', 'data',
sftfilepattern='data/*_glitch*.sft',
theta_prior=theta_prior, tref=tref, minStartTime=tstart, maxStartTime=tend,
nsteps=nsteps, nwalkers=nwalkers, ntemps=ntemps,
log10beta_min=log10beta_min)
mcmc.run()
mcmc.plot_corner(add_prior=True)
mcmc.print_summary()
import numpy as np
import pyfstat
outdir = 'data'
label = 'glitch_robust_search'
# Properties of the GW data
tstart = 1000000000
Tspan = 60 * 86400
# Fixed properties of the signal
F0s = 30
F1s = -1e-8
F2s = 0
Alpha = np.radians(83.6292)
Delta = np.radians(22.0144)
tref = tstart + .5 * Tspan
sftfilepattern = 'data/*glitching_signal*sft'
F0_width = np.sqrt(3)/(np.pi*Tspan)
F1_width = np.sqrt(45/4.)/(np.pi*Tspan**2)
DeltaF0 = 50 * F0_width
DeltaF1 = 50 * F1_width
theta_prior = {'F0': {'type': 'unif',
'lower': F0s-DeltaF0,
'upper': F0s+DeltaF0},
'F1': {'type': 'unif',
'lower': F1s-DeltaF1,
'upper': F1s+DeltaF1},
'F2': F2s,
'delta_F0': {'type': 'unif',
'lower': 0,
'upper': 1e-5},
'delta_F1': {'type': 'unif',
'lower': -1e-11,
'upper': 1e-11},
'tglitch': {'type': 'unif',
'lower': tstart+0.1*Tspan,
'upper': tstart+0.9*Tspan},
'Alpha': Alpha,
'Delta': Delta,
}
search = pyfstat.MCMCGlitchSearch(
label=label, outdir=outdir, sftfilepattern=sftfilepattern,
theta_prior=theta_prior, nglitch=1, tref=tref, nsteps=[500, 500],
ntemps=3, log10beta_min=-0.5, minStartTime=tstart,
maxStartTime=tstart+Tspan)
search.run()
search.plot_corner(label_offset=0.8, add_prior=True)
search.print_summary()
import numpy as np
import pyfstat
outdir = 'data'
label = 'simulated_glitching_signal'
# Properties of the GW data
tstart = 1000000000
Tspan = 60 * 86400
tref = tstart + .5 * Tspan
# Fixed properties of the signal
F0s = 30
F1s = -1e-8
F2s = 0
Alpha = np.radians(83.6292)
Delta = np.radians(22.0144)
h0 = 1e-25
sqrtSX = 1e-24
psi = -0.1
phi = 0
cosi = 0.5
# Glitch properties
dtglitch = 0.45 * Tspan # time (in secs) after minStartTime
dF0 = 5e-6
dF1 = 1e-12
detectors = 'H1'
glitch_data = pyfstat.Writer(
label=label, outdir=outdir, tref=tref, tstart=tstart,
F0=F0s, F1=F1s, F2=F2s, duration=Tspan, Alpha=Alpha,
Delta=Delta, sqrtSX=sqrtSX, dtglitch=dtglitch,
h0=h0, cosi=cosi, phi=phi, psi=psi,
delta_F0=dF0, delta_F1=dF1, add_noise=True)
glitch_data.make_data()
from pyfstat import Writer, GlitchWriter
import numpy as np
outdir = 'data'
# First, we generate data with a reasonably strong smooth signal
# Define parameters of the Crab pulsar as an example
......@@ -9,19 +10,19 @@ F1 = -1e-10
F2 = 0
Alpha = np.radians(83.6292)
Delta = np.radians(22.0144)
tref = 362750407.0
# Signal strength
h0 = 1e-23
h0 = 5e-24
# Properties of the GW data
sqrtSX = 1e-22
tstart = 1000000000
duration = 100*86400
tend = tstart+duration
tref = tstart + 0.5*duration
data = Writer(
label='basic', outdir='data', tref=tref, tstart=tstart, F0=F0, F1=F1,
label='0_glitch', outdir=outdir, tref=tref, tstart=tstart, F0=F0, F1=F1,
F2=F2, duration=duration, Alpha=Alpha, Delta=Delta, h0=h0, sqrtSX=sqrtSX)
data.make_data()
......@@ -31,11 +32,11 @@ print 'Predicted twoF value: {}\n'.format(twoF)
# Next, taking the same signal parameters, we include a glitch half way through
dtglitch = duration/2.0
delta_F0 = 4e-5
delta_F0 = 5e-6
delta_F1 = 0
glitch_data = GlitchWriter(
label='glitch', outdir='data', tref=tref, tstart=tstart, F0=F0, F1=F1,
label='1_glitch', outdir=outdir, tref=tref, tstart=tstart, F0=F0, F1=F1,
F2=F2, duration=duration, Alpha=Alpha, Delta=Delta, h0=h0, sqrtSX=sqrtSX,
dtglitch=dtglitch, delta_F0=delta_F0, delta_F1=delta_F1)
glitch_data.make_data()
......@@ -49,7 +50,7 @@ delta_F1 = [0, 0]
delta_F2 = [0, 0]
two_glitch_data = GlitchWriter(
label='twoglitch', outdir='data', tref=tref, tstart=tstart, F0=F0, F1=F1,
label='2_glitch', outdir=outdir, tref=tref, tstart=tstart, F0=F0, F1=F1,
F2=F2, duration=duration, Alpha=Alpha, Delta=Delta, h0=h0, sqrtSX=sqrtSX,
dtglitch=dtglitch, delta_phi=delta_phi, delta_F0=delta_F0,
delta_F1=delta_F1, delta_F2=delta_F2)
......
import pyfstat
F0 = 30.0
F1 = -1e-10
F2 = 0
Alpha = 5e-3
Delta = 6e-2
tref = 362750407.0
tstart = 1000000000
duration = 100*86400
tend = tstart + duration
theta_prior = {'F0': {'type': 'norm', 'loc': F0, 'scale': abs(1e-6*F0)},
'F1': {'type': 'norm', 'loc': F1, 'scale': abs(1e-6*F1)},
'F2': F2,
'Alpha': Alpha,
'Delta': Delta,
'delta_F0': {'type': 'halfnorm', 'loc': 0,
'scale': 1e-5*F0},
'delta_F1': 0,
'tglitch': {'type': 'unif',
'lower': tstart+0.1*duration,
'upper': tstart+0.9*duration},
}
ntemps = 4
log10beta_min = -1
nwalkers = 100
nsteps = [5000, 1000, 1000]
mcmc = pyfstat.MCMCGlitchSearch(
'semi_coherent_glitch_search_using_MCMC', 'data',
sftfilepattern='data/*_glitch*sft', theta_prior=theta_prior, tref=tref,
tstart=tstart, tend=tend, nsteps=nsteps, nwalkers=nwalkers,
scatter_val=1e-10, nglitch=1, ntemps=ntemps,
log10beta_min=log10beta_min)
mcmc.run()
mcmc.plot_corner(add_prior=True)
mcmc.print_summary()
import pyfstat
F0 = 30.0
F1 = -1e-10
F2 = 0
Alpha = 5e-3
Delta = 6e-2
tref = 362750407.0
tstart = 1000000000
duration = 100*86400
tend = tstart + duration
theta_prior = {'F0': {'type': 'norm', 'loc': F0, 'scale': abs(1e-6*F0)},
'F1': {'type': 'norm', 'loc': F1, 'scale': abs(1e-6*F1)},
'F2': F2,
'Alpha': Alpha,
'Delta': Delta,
'delta_F0_0': {'type': 'halfnorm', 'loc': 0,
'scale': 1e-7*F0},
'delta_F0_1': {'type': 'halfnorm', 'loc': 0,
'scale': 1e-7*F0},
'delta_F1_0': 0,
'delta_F1_1': 0,
'tglitch_0': {'type': 'unif',
'lower': tstart+0.01*duration,
'upper': tstart+0.5*duration},
'tglitch_1': {'type': 'unif',
'lower': tstart+0.5*duration,
'upper': tstart+0.99*duration},
}
nwalkers = 100
nsteps = [1000, 1000, 5000]
mcmc = pyfstat.MCMCGlitchSearch(
'semi_coherent_twoglitch_search', 'data', sftfilepattern='data/*twoglitch*sft',
theta_prior=theta_prior, tref=tref, tstart=tstart,
tend=tend, nsteps=nsteps, nwalkers=nwalkers, scatter_val=1e-10, nglitch=2)
mcmc.run()
mcmc.plot_corner(add_prior=True, tglitch_ratio=True, figsize=(10, 10))
mcmc.print_summary()
import numpy as np
import matplotlib.pyplot as plt
import pyfstat
from make_simulated_data import tstart, duration, tref, F0, F1, F2, Alpha, Delta, outdir
plt.style.use('paper')
label = 'semicoherent_glitch_robust_directed_MCMC_search_on_1_glitch'
Nstar = 100
F0_width = np.sqrt(Nstar)*np.sqrt(12)/(np.pi*duration)
F1_width = np.sqrt(Nstar)*np.sqrt(180)/(np.pi*duration**2)
theta_prior = {
'F0': {'type': 'unif',
'lower': F0-F0_width/2.,
'upper': F0+F0_width/2.},
'F1': {'type': 'unif',
'lower': F1-F1_width/2.,
'upper': F1+F1_width/2.},
'F2': F2,
'delta_F0': {'type': 'unif',
'lower': 0,
'upper': 1e-5},
'delta_F1': 0,
'tglitch': {'type': 'unif',
'lower': tstart+0.1*duration,
'upper': tstart+0.9*duration},
'Alpha': Alpha,
'Delta': Delta,
}
ntemps = 2
log10beta_min = -0.5
nwalkers = 100
nsteps = [500, 500]
mcmc = pyfstat.MCMCGlitchSearch(
label=label, sftfilepattern='data/*1_glitch*sft', theta_prior=theta_prior,
tref=tref, minStartTime=tstart, maxStartTime=tstart+duration,
nsteps=nsteps, nwalkers=nwalkers, ntemps=ntemps,
log10beta_min=log10beta_min, nglitch=1)
mcmc.transform_dictionary['F0'] = dict(
subtractor=F0, symbol='$f-f^\mathrm{s}$')
mcmc.transform_dictionary['F1'] = dict(
subtractor=F1, symbol='$\dot{f}-\dot{f}^\mathrm{s}$')
mcmc.run()
mcmc.plot_corner()
mcmc.print_summary()
import pyfstat
import numpy as np
import matplotlib.pyplot as plt
from make_simulated_data import tstart, duration, tref, F0, F1, F2, Alpha, Delta, outdir
try:
from gridcorner import gridcorner
except ImportError:
raise ImportError(
"Python module 'gridcorner' not found, please install from "
"https://gitlab.aei.uni-hannover.de/GregAshton/gridcorner")
label = 'semicoherent_glitch_robust_directed_grid_search_on_1_glitch'
plt.style.use('paper')
Nstar = 150
F0_width = np.sqrt(Nstar)*np.sqrt(12)/(np.pi*duration)
F1_width = np.sqrt(Nstar)*np.sqrt(180)/(np.pi*duration**2)
N = 61
F0s = [F0-F0_width/2., F0+F0_width/2., F0_width/N]
F1s = [F1-F1_width/2., F1+F1_width/2., F1_width/N]
F2s = [F2]
Alphas = [Alpha]
Deltas = [Delta]
max_delta_F0 = 1e-5
tglitchs = [tstart+0.1*duration, tstart+0.9*duration, 0.8*float(duration)/N]
delta_F0s = [0, max_delta_F0, max_delta_F0/N]
delta_F1s = [0]
search = pyfstat.GridGlitchSearch(
label, outdir, 'data/*1_glitch*sft', F0s=F0s, F1s=F1s, F2s=F2s,
Alphas=Alphas, Deltas=Deltas, tref=tref, minStartTime=tstart,
maxStartTime=tstart+duration, tglitchs=tglitchs, delta_F0s=delta_F0s,
delta_F1s=delta_F1s)
search.run()
F0_vals = np.unique(search.data[:, 0]) - F0
F1_vals = np.unique(search.data[:, 1]) - F1
delta_F0s_vals = np.unique(search.data[:, 5])
tglitch_vals = np.unique(search.data[:, 7])
tglitch_vals_days = (tglitch_vals-tstart) / 86400.
twoF = search.data[:, -1].reshape((len(F0_vals), len(F1_vals),
len(delta_F0s_vals), len(tglitch_vals)))
xyz = [F0_vals, F1_vals, delta_F0s_vals, tglitch_vals_days]
labels = ['$f - f_0$\n[Hz]', '$\dot{f} - \dot{f}_0$\n[Hz/s]',
'$\delta f$\n[Hz]', '$t^g_0$\n[days]', '$\widehat{2\mathcal{F}}$']
fig, axes = gridcorner(
twoF, xyz, projection='log_mean', whspace=0.1, factor=1.2, labels=labels)
fig.savefig('{}/{}_projection_matrix.png'.format(outdir, label),
bbox_inches='tight')
import numpy as np
import matplotlib.pyplot as plt
import pyfstat
from make_simulated_data import tstart, duration, tref, F0, F1, F2, Alpha, Delta, outdir
plt.style.use('paper')
label = 'standard_directed_MCMC_search_on_1_glitch'
Nstar = 10000
F0_width = np.sqrt(Nstar)*np.sqrt(12)/(np.pi*duration)
F1_width = np.sqrt(Nstar)*np.sqrt(180)/(np.pi*duration**2)
theta_prior = {
'F0': {'type': 'unif',
'lower': F0-F0_width/2.,
'upper': F0+F0_width/2.},
'F1': {'type': 'unif',
'lower': F1-F1_width/2.,
'upper': F1+F1_width/2.},
'F2': F2,
'Alpha': Alpha,
'Delta': Delta,
}
ntemps = 2
log10beta_min = -0.5
nwalkers = 100
nsteps = [500, 2000]
mcmc = pyfstat.MCMCSearch(
label=label, sftfilepattern='data/*1_glitch*sft', theta_prior=theta_prior,
tref=tref, minStartTime=tstart, maxStartTime=tstart+duration,
nsteps=nsteps, nwalkers=nwalkers, ntemps=ntemps,
log10beta_min=log10beta_min)
mcmc.transform_dictionary['F0'] = dict(
subtractor=F0, symbol='$f-f^\mathrm{s}$')
mcmc.transform_dictionary['F1'] = dict(
subtractor=F1, symbol='$\dot{f}-\dot{f}^\mathrm{s}$')
mcmc.run()
mcmc.plot_corner()
mcmc.print_summary()
import pyfstat
import numpy as np
import matplotlib.pyplot as plt
from projection_matrix import projection_matrix
plt.style.use('paper')
try:
from gridcorner import gridcorner
except ImportError:
raise ImportError(
"Python module 'gridcorner' not found, please install from "
"https://gitlab.aei.uni-hannover.de/GregAshton/gridcorner")
F0 = 30.0
F1 = 1e-10
......@@ -55,6 +59,6 @@ twoF = search.data[:, -1].reshape((len(F0_vals), len(F1_vals), len(F2_vals)))
xyz = [F0_vals, F1_vals, F2_vals]
labels = ['$f - f_0$', '$\dot{f} - \dot{f}_0$', '$\ddot{f} - \ddot{f}_0$',
'$\widetilde{2\mathcal{F}}$']
fig, axes = projection_matrix(twoF, xyz, projection='log_mean', labels=labels,
whspace=0.1, factor=1.8)
fig, axes = gridcorner(
twoF, xyz, projection='log_mean', labels=labels, whspace=0.1, factor=1.8)
fig.savefig('{}/{}_projection_matrix.png'.format(outdir, label))
......@@ -2,8 +2,6 @@ import pyfstat
import numpy as np
import matplotlib.pyplot as plt
plt.style.use('paper')
F0 = 30.0
F1 = 0
F2 = 0
......
......@@ -56,7 +56,7 @@ mcmc = pyfstat.MCMCSearch(
sftfilepattern='data/*'+data_label+'*sft', theta_prior=theta_prior, tref=tref,
minStartTime=tstart, maxStartTime=tend, nsteps=nsteps, nwalkers=nwalkers,
ntemps=ntemps, log10beta_min=log10beta_min)
mcmc.run(context='paper', subtractions=[30, -1e-10])
mcmc.run()
mcmc.plot_corner(add_prior=True)
mcmc.print_summary()
......
......@@ -2,8 +2,6 @@ import pyfstat
import numpy as np
import matplotlib.pyplot as plt
plt.style.use('./paper-style.mplstyle')
F0 = 30.0
F1 = -1e-10
F2 = 0
......@@ -63,8 +61,8 @@ NstarMax = 1000
Nsegs0 = 100
fig, axes = plt.subplots(nrows=2, figsize=(3.4, 3.5))
fig, axes = mcmc.run(
NstarMax=NstarMax, Nsegs0=Nsegs0, subtractions=[F0, F1], labelpad=0.01,
plot_det_stat=False, return_fig=True, context='paper', fig=fig,
NstarMax=NstarMax, Nsegs0=Nsegs0, labelpad=0.01,
plot_det_stat=False, return_fig=True, fig=fig,
axes=axes)
for ax in axes:
ax.grid()
......
......@@ -58,6 +58,9 @@ mcmc = pyfstat.MCMCSemiCoherentSearch(
theta_prior=theta_prior, tref=tref, minStartTime=tstart, maxStartTime=tend,
nsteps=nsteps, nwalkers=nwalkers, ntemps=ntemps,
log10beta_min=log10beta_min)
mcmc.transform_dictionary = dict(
F0=dict(subtractor=F0, symbol='$f-f^\mathrm{s}$'),
F1=dict(subtractor=F1, symbol='$\dot{f}-\dot{f}^\mathrm{s}$'))
mcmc.run()
mcmc.plot_corner(add_prior=True)
mcmc.print_summary()
......@@ -25,9 +25,7 @@ theta_prior = {'F0': {'type': 'unif',
'F2': F2,
'Alpha': Alpha,
'Delta': Delta,
'transient_tstart': {'type': 'unif',
'lower': minStartTime,
'upper': maxStartTime},
'transient_tstart': minStartTime,
'transient_duration': {'type': 'halfnorm',
'loc': 0.001*Tspan,
'scale': 0.5*Tspan}
......@@ -39,11 +37,12 @@ nwalkers = 100
nsteps = [100, 100]
mcmc = pyfstat.MCMCTransientSearch(
label='transient_search', outdir='data',
sftfilepattern='data/*simulated_transient_signal*sft',
label='transient_search', outdir='data_l',
sftfilepattern='data_l/*simulated_transient_signal*sft',
theta_prior=theta_prior, tref=tref, minStartTime=minStartTime,
maxStartTime=maxStartTime, nsteps=nsteps, nwalkers=nwalkers, ntemps=ntemps,
log10beta_min=log10beta_min)
log10beta_min=log10beta_min,
transientWindowType='rect')
mcmc.run()
mcmc.plot_corner(label_offset=0.7)
mcmc.print_summary()
......@@ -19,8 +19,8 @@ h0 = 1e-23
sqrtSX = 1e-22
transient = pyfstat.Writer(
label='simulated_transient_signal', outdir='data', tref=tref,
label='simulated_transient_signal', outdir='data_l', tref=tref,
tstart=transient_tstart, F0=F0, F1=F1, F2=F2, duration=transient_duration,
Alpha=Alpha, Delta=Delta, h0=h0, sqrtSX=sqrtSX, minStartTime=minStartTime,
maxStartTime=maxStartTime)
maxStartTime=maxStartTime, transientWindowType='rect')
transient.make_data()
#!/usr/bin/env python
import pyfstat
F0 = 30.0
F1 = -1e-10
F2 = 0
Alpha = 0.5
Delta = 1
minStartTime = 1000000000
maxStartTime = minStartTime + 2*86400
Tspan = maxStartTime - minStartTime
tref = minStartTime
Tsft = 1800
DeltaF0 = 1e-2
DeltaF1 = 1e-9
theta_prior = {'F0': {'type': 'unif',
'lower': F0-DeltaF0/2.,
'upper': F0+DeltaF0/2.},
'F1': {'type': 'unif',
'lower': F1-DeltaF1/2.,
'upper': F1+DeltaF1/2.},
'F2': F2,
'Alpha': Alpha,
'Delta': Delta,
'transient_tstart': {'type': 'unif',
'lower': minStartTime,
'upper': maxStartTime-2*Tsft},
'transient_duration': {'type': 'unif',
'lower': 2*Tsft,
'upper': Tspan-2*Tsft}
}
ntemps = 2
log10beta_min = -1
nwalkers = 100
nsteps = [100, 100]
mcmc = pyfstat.MCMCTransientSearch(
label='transient_search', outdir='data_s',
sftfilepattern='data_s/*simulated_transient_signal*sft',
theta_prior=theta_prior, tref=tref, minStartTime=minStartTime,
maxStartTime=maxStartTime, nsteps=nsteps, nwalkers=nwalkers, ntemps=ntemps,
log10beta_min=log10beta_min,
transientWindowType='rect')
mcmc.run()
mcmc.plot_corner(label_offset=0.7)
mcmc.print_summary()
#!/usr/bin/env python
import pyfstat
import os
import numpy as np
import matplotlib.pyplot as plt
datadir = 'data_s'
F0 = 30.0
F1 = -1e-10
F2 = 0
Alpha = 0.5
Delta = 1
minStartTime = 1000000000
maxStartTime = minStartTime + 2*86400
Tspan = maxStartTime - minStartTime
tref = minStartTime
Tsft = 1800
m = 0.001
dF0 = np.sqrt(12*m)/(np.pi*Tspan)
DeltaF0 = 100*dF0
F0s = [F0-DeltaF0/2., F0+DeltaF0/2., dF0]
F1s = [F1]
F2s = [F2]
Alphas = [Alpha]
Deltas = [Delta]
print('Standard CW search:')
search1 = pyfstat.GridSearch(
label='CW', outdir=datadir,
sftfilepattern=os.path.join(datadir,'*simulated_transient_signal*sft'),
F0s=F0s, F1s=F1s, F2s=F2s, Alphas=Alphas, Deltas=Deltas, tref=tref,
minStartTime=minStartTime, maxStartTime=maxStartTime,
BSGL=False,
outputTransientFstatMap=True)
search1.run()
search1.print_max_twoF()
search1.plot_1D(xkey='F0',
xlabel='freq [Hz]', ylabel='$2\mathcal{F}$')
print('with t0,tau bands:')
search2 = pyfstat.GridSearch(
label='tCW', outdir=datadir,
sftfilepattern=os.path.join(datadir,'*simulated_transient_signal*sft'),
F0s=F0s, F1s=F1s, F2s=F2s, Alphas=Alphas, Deltas=Deltas, tref=tref,
minStartTime=minStartTime, maxStartTime=maxStartTime,
transientWindowType='rect', t0Band=Tspan-2*Tsft, tauBand=Tspan,
BSGL=False,
outputTransientFstatMap=True)
search2.run()
search2.print_max_twoF()
search2.plot_1D(xkey='F0',
xlabel='freq [Hz]', ylabel='$2\mathcal{F}$')
0% Loading or .
You are about to add 0 people to the discussion. Proceed with caution.
Please register or to comment