forked from masonng-astro/nicerpy_xrayanalysis
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Lv2_phase.py
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Lv2_phase.py
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#!/usr/bin/env python
# -*- coding: utf-8 -*-
"""
Created on Mon Jan 14 9:56am 2019
Plotting phase curves
Updated on Mon Jun 3 - Added name_par_list for NICERsoft segments
"""
from __future__ import division, print_function
from astropy.io import fits
import numpy as np
import Lv0_dirs,Lv0_fits2dict,Lv1_data_bin,Lv2_mkdir
from scipy import stats
from pint.eventstats import sf_z2m,z2m,sig2sigma
from PyAstronomy.pyasl import foldAt
import pathlib
import matplotlib.gridspec as gridspec
import matplotlib.pyplot as plt
import os
Lv0_dirs.global_par() #obtaining the global parameters
def pulse_profile(f_pulse,times,counts,shift,no_phase_bins):
"""
Calculating the pulse profile for the observation. Goes from 0 to 2!
Thoughts on 1/14/2020: I wonder if the count rate is calculated from times[-1]-times[0]?
If so, this is WRONG! I should be using the total from the GTIs!
f_pulse - the frequency of the pulse
times - the array of time values
counts - the array of counts values
shift - how much to shift the pulse by in the phase axis.
It only affects how it is presented.
no_phase_bins - number of phase bins desired
"""
period = 1/f_pulse
phases = foldAt(times,period,T0=shift*period)
index_sort = np.argsort(phases)
phases = list(phases[index_sort]) + list(phases[index_sort]+1)
counts = list(counts[index_sort])*2
phase_bins = np.linspace(0,2,no_phase_bins*2+1)
summed_profile, bin_edges, binnumber = stats.binned_statistic(phases,counts,statistic='mean',bins=phase_bins)
return phases, phase_bins, summed_profile
def phase_exposure(start_time, stop_time, period, nbin=16, gtis=None):
"""Calculate the exposure on each phase of a pulse profile.
THIS FUNCTION IS FROM STINGRAY.
https://stingray.readthedocs.io/en/latest/_modules/stingray/pulse/pulsar.html
(as of 6/29/2020)
Parameters
----------
start_time, stop_time : float
Starting and stopping time (or phase if ``period==1``)
period : float
The pulse period (if 1, equivalent to phases)
Other parameters
----------------
nbin : int, optional, default 16
The number of bins in the profile
gtis : [[gti00, gti01], [gti10, gti11], ...], optional, default None
Good Time Intervals
Returns
-------
expo : array of floats
The normalized exposure of each bin in the pulse profile (1 is the
highest exposure, 0 the lowest)
"""
if gtis is None:
gtis = np.array([[start_time, stop_time]])
# Use precise floating points -------------
start_time = np.longdouble(start_time)
stop_time = np.longdouble(stop_time)
period = np.longdouble(period)
gtis = np.array(gtis, dtype=np.longdouble)
# -----------------------------------------
expo = np.zeros(nbin)
phs = np.linspace(0, 1, nbin + 1)
phs = np.array(list(zip(phs[0:-1], phs[1:])))
# Discard gtis outside [start, stop]
good = np.logical_and(gtis[:, 0] < stop_time, gtis[:, 1] > start_time)
gtis = gtis[good]
for g in gtis:
g0 = g[0]
g1 = g[1]
if g0 < start_time:
# If the start of the fold is inside a gti, start from there
g0 = start_time
if g1 > stop_time:
# If the end of the fold is inside a gti, end there
g1 = stop_time
length = g1 - g0
# How many periods inside this length?
nraw = length / period
# How many integer periods?
nper = nraw.astype(int)
# First raw exposure: the number of periods
expo += nper / nbin
# FRACTIONAL PART =================
# What remains is additional exposure for part of the profile.
start_phase = np.fmod(g0 / period, 1)
end_phase = nraw - nper + start_phase
limits = [[start_phase, end_phase]]
# start_phase is always < 1. end_phase not always. In this case...
if end_phase > 1:
limits = [[0, end_phase - 1], [start_phase, 1]]
for l in limits:
l0 = l[0]
l1 = l[1]
# Discards bins untouched by these limits
goodbins = np.logical_and(phs[:, 0] <= l1, phs[:, 1] >= l0)
idxs = np.arange(len(phs), dtype=int)[goodbins]
for i in idxs:
start = np.max([phs[i, 0], l0])
stop = np.min([phs[i, 1], l1])
w = stop - start
expo[i] += w
return expo / np.max(expo)
def pulse_folding(t,T,T0,f,fdot,fdotdot,no_phase_bins,mission):
"""
Calculating the pulse profile by also incorporating \dot{f} corrections!
Goes from 0 to 2.
t - array of time values
T - sum of all the GTIs
T0 - reference epoch in MJD
f - pulse/folding Frequency
fdot - frequency derivative
fdotdot - second derivative of frequency
no_phase_bins - number of phase bins desired (recommended 20!)
mission - "NICER", "XMM", or "SWIFT" for now
Returns the pulse profile in counts/s/phase bin vs phase. The number of counts
is divided by the exposure time (calculated through total sum of the GTIs)
Also added a "TIMEZERO" manually in the script since it'd be inconvenient to call the eventfile here.
"""
if mission == "NICER":
##### NICER
MJDREFI = 56658.0
MJDREFF = 0.000777592592592593
TIMEZERO = -1
t_MJDs = MJDREFI + MJDREFF + (TIMEZERO+t)/86400 #Swift or NICER
if mission == "SWIFT":
##### SWIFT
MJDREFI = 51910.0
MJDREFF = 7.428703700000000E-04
TIMEZERO = 0
t_MJDs = MJDREFI + MJDREFF + (TIMEZERO+t)/86400 #Swift or NICER
if mission == "XMM":
##### XMM-NEWTON
MJDREF = 50814.0
t_MJDs = MJDREF + t/86400.0
tau = (t_MJDs-T0)*86400.0
#print(tau[:10])
#print(f*tau[:10])
phase = (f*tau + fdot/2 *tau**2 + fdotdot/6*tau**3)%1
#print(phase[:10])
counts = np.ones(len(phase))
phase_bins = np.linspace(0,1,no_phase_bins+1)
summed_profile,bin_edges,binnumber = stats.binned_statistic(phase,counts,statistic='sum',bins=phase_bins)
phase_bins_total = np.array(list(phase_bins[:-1]) + list(phase_bins+1))
summed_profile_total = np.array(list(summed_profile)*2)
error = np.sqrt(summed_profile_total)
return phase_bins_total, summed_profile_total/T, error/T #/T
#return phase_bins_total, summed_profile_total, error
def get_Z2(phases,m):
"""
Calculate the Z^2 significances given the event file and harmonic number m
eventfile - name of event file
m - number of harmonics
"""
z_vals = z2m(phases,m=m)
probs = sf_z2m(z_vals)
significances = sig2sigma(probs)
return significances
def get_chi2(profile,error):
"""
Calculating the chi^2 value from the folded profile
phase - array of phase values
profile - flux/counts per sec per phase bin
error - corresponding errors
"""
mean_prof = np.mean(profile)
return sum( (profile-mean_prof)**2/error**2 )
def whole(eventfile,par_list,tbin_size,pulse_pars,shift,no_phase_bins,mode):
"""
Plot the entire raw pulse profile without any cuts to the data.
eventfile - path to the event file. Will extract ObsID from this for the NICER files.
par_list - A list of parameters we'd like to extract from the FITS file
(e.g., from eventcl, PI_FAST, TIME, PI,)
tbin_size - the size of the time bins (in seconds!)
>> e.g., tbin_size = 2 means bin by 2s
>> e.g., tbin_size = 0.05 means bin by 0.05s!
pulse_pars - parameters corresponding to the pulse
shift - how much to shift the pulse by in the phase axis.
It only affects how the pulse profile is 'displaced'.
no_phase_bins - number of phase bins desired
mode - whether we want to show or save the plot.
pulse_pars will have [f,fdot,fdotdot]
"""
if type(eventfile) != str:
raise TypeError("eventfile should be a string!")
if type(pulse_pars) != list and type(pulse_pars) != np.ndarray:
raise TypeError("pulse_pars should either be a list or an array!")
if 'TIME' not in par_list:
raise ValueError("You should have 'TIME' in the parameter list!")
if type(par_list) != list and type(par_list) != np.ndarray:
raise TypeError("par_list should either be a list or an array!")
if mode != 'show' and mode != 'save' and mode != 'overlap':
raise ValueError("Mode should either be 'show' or 'save' or 'overlap'!")
parent_folder = str(pathlib.Path(eventfile).parent)
data_dict = Lv0_fits2dict.fits2dict(eventfile,1,par_list)
gtis = Lv0_fits2dict.fits2dict(eventfile,2,['START','STOP'])
T = sum([ (gtis['STOP'][i]-gtis['START'][i]) for i in range(len(gtis['START'])) ])
times = data_dict['TIME']
if pulse_pars[1] == 0 and pulse_pars[2] == 0: #i.e., if both \dot{f} and \ddot{f} are zero; that is, if we have no frequency derivatives
counts = np.ones(len(times))
shifted_t = times-times[0]
t_bins = np.linspace(0,np.ceil(shifted_t[-1]),int(np.ceil(shifted_t[-1])*1/tbin_size+1))
summed_data, bin_edges, binnumber = stats.binned_statistic(shifted_t,counts,statistic='sum',bins=t_bins) #binning the time values in the data
phases, phase_bins, summed_profile = pulse_profile(pulse_pars[0],t_bins[:-1],summed_data,shift,no_phase_bins)
else:
phase_bins, summed_profile = pulse_folding(times,T,times[0],pulse_pars[0],pulse_pars[1],pulse_pars[2],no_phase_bins)
event_header = fits.open(eventfile)[1].header
obj_name = event_header['OBJECT']
obsid = event_header['OBS_ID']
if mode != 'overlap':
plt.figure()
plt.title('Pulse profile for ' + obj_name + ', ObsID ' + str(obsid),fontsize=12)
# plt.plot(phase_bins[:-1],summed_profile*(times[-1]-times[0])/T)
plt.step(phase_bins[:-1],summed_profile*(times[-1]-times[0])/T)
plt.xlabel('Phase', fontsize=12)
plt.ylabel('Count/' + str(tbin_size) + 's',fontsize=12)
if mode == 'show':
plt.show()
elif mode == 'save':
filename = 'pp_' + obsid + '_bin' + str(tbin_size) + 's.pdf'
plt.savefig(parent_folder+'/'+filename,dpi=900)
plt.close()
return phase_bins[:-1],summed_profile
def partial_t(eventfile,par_list,tbin_size,pulse_pars,shift,no_phase_bins,t1,t2,mode):
"""
Plot the pulse profile for a desired time interval.
eventfile - path to the event file. Will extract ObsID from this for the NICER files.
par_list - A list of parameters we'd like to extract from the FITS file
(e.g., from eventcl, PI_FAST, TIME, PI,)
tbin_size - the size of the time bins (in seconds!)
>> e.g., tbin_size = 2 means bin by 2s
>> e.g., tbin_size = 0.05 means bin by 0.05s!
pulse_pars - parameters corresponding to the pulse
shift - how much to shift the pulse by in the phase axis.
It only affects how it is presented.
no_phase_bins - number of phase bins desired
t1 - lower time boundary
t2 - upper time boundary
mode - whether we want to show or save the plot
pulse_pars will have [f,fdot,fdotdot]
"""
if type(eventfile) != str:
raise TypeError("eventfile should be a string!")
if type(pulse_pars) != list and type(pulse_pars) != np.ndarray:
raise TypeError("pulse_pars should either be a list or an array!")
if 'TIME' not in par_list:
raise ValueError("You should have 'TIME' in the parameter list!")
if type(par_list) != list and type(par_list) != np.ndarray:
raise TypeError("par_list should either be a list or an array!")
if t2<t1:
raise ValueError("t2 should be greater than t1!")
if mode != 'show' and mode != 'save' and mode != 'overlap':
raise ValueError("Mode should either be 'show' or 'save' or 'overlap'!")
parent_folder = str(pathlib.Path(eventfile).parent)
data_dict = Lv0_fits2dict.fits2dict(eventfile,1,par_list)
gtis = Lv0_fits2dict.fits2dict(eventfile,2,['START','STOP'])
T = sum([ (gtis['STOP'][i]-gtis['START'][i]) for i in range(len(gtis['START'])) ])
if pulse_pars[1] == 0 and pulse_pars[2] == 0:
truncated_t, truncated_counts = Lv1_data_bin.binning_t(eventfile,par_list,tbin_size,t1,t2)
phases, phase_bins, summed_profile = pulse_profile(pulse_pars[0],truncated_t[:-1],truncated_counts,shift,no_phase_bins)
else:
truncated_t, truncated_counts = Lv1_data_bin.binning_t(eventfile,par_list,tbin_size,t1,t2)
phase_bins, summed_profile = pulse_folding(truncated_t,T,0,pulse_pars[0],pulse_pars[1],pulse_pars[2],no_phase_bins)
event_header = fits.open(eventfile)[1].header
obj_name = event_header['OBJECT']
obsid = event_header['OBS_ID']
if mode != 'overlap':
plt.figure()
plt.title('Pulse profile for ' + obj_name + ', ObsID ' + str(obsid) + '\n Time interval: ' + str(t1) + 's - ' + str(t2) + 's',fontsize=12)
# plt.plot(phase_bins[:-1], summed_profile*(times[-1]-times[0])/T)
plt.step(phase_bins[:-1],summed_profile*(times[-1]-times[0])/T)
plt.xlabel('Phase', fontsize=12)
plt.ylabel('Count/' + str(tbin_size) + 's',fontsize=12)
if mode == 'show':
plt.show()
elif mode == 'save':
filename = 'pp_' + obsid + '_bin' + str(tbin_size) + 's_' + str(t1) + 's-' + str(t2) + 's.pdf'
plt.savefig(parent_folder+'/'+filename,dpi=900)
plt.close()
return phase_bins[:-1],summed_profile
def partial_E(eventfile,par_list,tbin_size,Ebin_size,pulse_pars,shift,no_phase_bins,E1,E2,mode):
"""
Plot the pulse profile for a desired energy range.
[Though I don't think this will be used much. Count/s vs energy is pointless,
since we're not folding in response matrix information here to get the flux.
So we're just doing a count/s vs time with an energy cut to the data.]
INTERJECTION: This caveat is for the spectrum, NOT the pulse profile!
eventfile - path to the event file. Will extract ObsID from this for the NICER files.
par_list - A list of parameters we'd like to extract from the FITS file
(e.g., from eventcl, PI_FAST, TIME, PI,)
tbin_size - the size of the time bins (in seconds!)
>> e.g., tbin_size = 2 means bin by 2s
>> e.g., tbin_size = 0.05 means by in 0.05s
Ebin_size - the size of the energy bins (in keV!)
>> e.g., Ebin_size = 0.1 means bin by 0.1keV
>> e.g., Ebin_size = 0.01 means bin by 0.01keV!
pulse_pars - parameters corresponding to the pulse
shift - how much to shift the pulse by in the phase axis.
It only affects how it is presented.
no_phase_bins - number of phase bins desired
E1 - lower energy boundary
E2 - upper energy boundary
pulse_pars will have [f,fdot,fdotdot]
"""
if type(eventfile) != str:
raise TypeError("eventfile should be a string!")
if type(pulse_pars) != list and type(pulse_pars) != np.ndarray:
raise TypeError("pulse_pars should either be a list or an array!")
if 'TIME' not in par_list:
raise ValueError("You should have 'TIME' in the parameter list!")
if type(par_list) != list and type(par_list) != np.ndarray:
raise TypeError("par_list should either be a list or an array!")
if E2<E1:
raise ValueError("E2 should be greater than E1!")
if mode != 'show' and mode != 'save' and mode != 'overlap':
raise ValueError("Mode should either be 'show' or 'save' or 'overlap'!")
parent_folder = str(pathlib.Path(eventfile).parent)
data_dict = Lv0_fits2dict.fits2dict(eventfile,1,par_list)
gtis = Lv0_fits2dict.fits2dict(eventfile,2,['START','STOP'])
T = sum([ (gtis['STOP'][i]-gtis['START'][i]) for i in range(len(gtis['START'])) ])
if pulse_pars[1] == 0 and pulse_pars[2] == 0:
truncated_t, truncated_t_counts, truncated_E, truncated_E_counts = Lv1_data_bin.binning_E(eventfile,par_list,tbin_size,Ebin_size,E1,E2)
phases, phase_bins, summed_profile = pulse_profile(pulse_pars[0],truncated_t[:-1],truncated_t_counts,shift,no_phase_bins)
else:
phase_bins, summed_profile = pulse_folding(truncated_t,T,0,pulse_pars[0],pulse_pars[1],pulse_pars[2],no_phase_bins)
event_header = fits.open(eventfile)[1].header
obj_name = event_header['OBJECT']
obsid = event_header['OBS_ID']
if mode != 'overlap':
plt.figure()
# plt.plot(phase_bins[:-1], summed_profile*(times[-1]-times[0])/T,'-')
# print(sum(summed_profile)/truncated_t[-1])
plt.step(phase_bins[:-1],summed_profile*(times[-1]-times[0])/T)
plt.xlabel('Phase', fontsize=12)
plt.ylabel('Count/' + str(tbin_size) + 's',fontsize=12)
if mode != 'overlap':
plt.title('Pulse profile for ' + obj_name + ', ObsID ' + str(obsid)+ '\n Energy range: ' + str(E1) + 'keV - ' + str(E2) + 'keV',fontsize=12)
if mode == 'show':
plt.show()
elif mode == 'save':
filename = 'pp_' + obsid + '_bin' + str(tbin_size) + 's_' + str(E1) + 'keV-' + str(E2) + 'keV.pdf'
plt.savefig(parent_folder+'/'+filename,dpi=900)
plt.close()
return phase_bins[:-1],summed_profile
def partial_tE(eventfile,par_list,tbin_size,Ebin_size,pulse_pars,shift,no_phase_bins,t1,t2,E1,E2,mode):
"""
Plot the pulse profile for a desired time interval and desired energy range.
eventfile - path to the event file. Will extract ObsID from this for the NICER files.
par_list - A list of parameters we'd like to extract from the FITS file
(e.g., from eventcl, PI_FAST, TIME, PI,)
tbin_size - the size of the time bins (in seconds!)
>> e.g., tbin_size = 2 means bin by 2s
>> e.g., tbin_size = 0.05 means by in 0.05s
Ebin_size - the size of the energy bins (in keV!)
>> e.g., Ebin_size = 0.1 means bin by 0.1keV
>> e.g., Ebin_size = 0.01 means bin by 0.01keV!
pulse_pars - parameters corresponding to the pulse
shift - how much to shift the pulse by in the phase axis.
It only affects how it is presented.
no_phase_bins - number of phase bins desired
t1 - lower time boundary
t2 - upper time boundary
E1 - lower energy boundary
E2 - upper energy boundary
mode - whether we want to show or save the plot
pulse_pars will have [f,fdot,fdotdot]
"""
if type(eventfile) != str:
raise TypeError("eventfile should be a string!")
if type(pulse_pars) != list and type(pulse_pars) != np.ndarray:
raise TypeError("pulse_pars should either be a list or an array!")
if 'TIME' not in par_list:
raise ValueError("You should have 'TIME' in the parameter list!")
if type(par_list) != list and type(par_list) != np.ndarray:
raise TypeError("par_list should either be a list or an array!")
if E2<E1:
raise ValueError("E2 should be greater than E1!")
if t2<t1:
raise ValueError("t2 should be greater than t1!")
if mode != 'show' and mode != 'save':
raise ValueError("Mode should either be 'show' or 'save'!")
parent_folder = str(pathlib.Path(eventfile).parent)
data_dict = Lv0_fits2dict.fits2dict(eventfile,1,par_list)
gtis = Lv0_fits2dict.fits2dict(eventfile,2,['START','STOP'])
T = sum([ (gtis['STOP'][i]-gtis['START'][i]) for i in range(len(gtis['START'])) ])
if pulse_pars[1] == 0 and pulse_pars[2] == 0:
truncated_t, truncated_t_counts, truncated_E, truncated_E_counts = Lv1_data_bin.binning_tE(eventfile,par_list,tbin_size,Ebin_size,t1,t2,E1,E2)
phases, phase_bins, summed_profile = pulse_profile(pulse_pars[0],truncated_t[:-1],truncated_t_counts,shift,no_phase_bins)
else:
phase_bins, summed_profile = pulse_folding(truncated_t,T,0,pulse_pars[0],pulse_pars[1],pulse_pars[2],no_phase_bins)
event_header = fits.open(eventfile)[1].header
obj_name = event_header['OBJECT']
obsid = event_header['OBS_ID']
if mode != 'overlap':
plt.figure()
plt.title('Pulse profile for ' + obj_name + ', ObsID ' + str(obsid)+ '\n Time interval: ' + str(t1) + 's - ' + str(t2) + 's'+ '\n Energy range: ' + str(E1) + 'keV - ' + str(E2) + 'keV',fontsize=12)
# plt.plot(phase_bins[:-1], summed_profile*(times[-1]-times[0])/T)
plt.step(phase_bins[:-1],summed_profile*(times[-1]-times[0])/T)
plt.xlabel('Phase', fontsize=12)
plt.ylabel('Count/' + str(tbin_size) + 's',fontsize=12)
if mode == 'show':
plt.show()
elif mode == 'save':
filename = 'pp_' + obsid + '_bin' + str(tbin_size) + 's_' + str(t1) + 's-' + str(t2) + 's_' + str(E1) + 'keV-' + str(E2) + 'keV.pdf'
plt.savefig(parent_folder+'/'+filename,dpi=900)
plt.close()
return phase_bins[:-1],summed_profile
################################################################################
### SUBPLOTS
def partial_subplots_E(eventfile,par_list,tbin_size,Ebin_size,f_pulse,shift,no_phase_bins,subplot_Es,E1,E2,mode):
"""
Plot the pulse profile for a desired energy range.
[Though I don't think this will be used much. Count/s vs energy is pointless,
since we're not folding in response matrix information here to get the flux.
So we're just doing a count/s vs time with an energy cut to the data.]
INTERJECTION: This caveat is for the spectrum, NOT the pulse profile!
eventfile - path to the event file. Will extract ObsID from this for the NICER files.
par_list - A list of parameters we'd like to extract from the FITS file
(e.g., from eventcl, PI_FAST, TIME, PI,)
tbin_size - the size of the time bins (in seconds!)
>> e.g., tbin_size = 2 means bin by 2s
>> e.g., tbin_size = 0.05 means by in 0.05s
Ebin_size - the size of the energy bins (in keV!)
>> e.g., Ebin_size = 0.1 means bin by 0.1keV
>> e.g., Ebin_size = 0.01 means bin by 0.01keV!
f_pulse - the frequency of the pulse
shift - how much to shift the pulse by in the phase axis.
It only affects how it is presented.
no_phase_bins - number of phase bins desired
subplot_Es - list of tuples defining energy boundaries for pulse profiles
E1 - lower energy boundary
E2 - upper energy boundary
"""
if type(eventfile) != str:
raise TypeError("eventfile should be a string!")
if 'TIME' not in par_list:
raise ValueError("You should have 'TIME' in the parameter list!")
if type(par_list) != list and type(par_list) != np.ndarray:
raise TypeError("par_list should either be a list or an array!")
if E2<E1:
raise ValueError("E2 should be greater than E1!")
if mode != 'show' and mode != 'save' and mode != 'overlap':
raise ValueError("Mode should either be 'show' or 'save' or 'overlap'!")
parent_folder = str(pathlib.Path(eventfile).parent)
#should find a way to generalize calling p10,p20,etc in the future..!
fig,(p10,p20,p30,p40,p50,p60) = plt.subplots(6,1)
gs = gridspec.GridSpec(6,1)
for i in range(len(subplot_Es)): #for each tuple of energy boundaries
truncated_t, truncated_t_counts, truncated_E, truncated_E_counts = Lv1_data_bin.binning_E(eventfile,par_list,tbin_size,Ebin_size,subplot_Es[i][0],subplot_Es[i][1])
phases, phase_bins, summed_profile = pulse_profile(pulse_pars[0],truncated_t[:-1],truncated_t_counts,shift,no_phase_bins)
plt.subplot(gs[i]).plot(phase_bins[:-1],summed_profile,'-')
event_header = fits.open(eventfile)[1].header
obj_name = event_header['OBJECT']
obsid = event_header['OBS_ID']
fig.suptitle(str(obsid),fontsize=12)
if mode != 'overlap':
plt.figure()
plt.xlabel('Phase', fontsize=12)
plt.ylabel('Count/' + str(tbin_size) + 's',fontsize=12)
if mode != 'overlap':
plt.title('Pulse profile for ' + obj_name + ', ObsID ' + str(obsid)+ '\n Energy range: ' + str(E1) + 'keV - ' + str(E2) + 'keV',fontsize=12)
if mode == 'show':
plt.show()
elif mode == 'save':
filename = 'pp_subplots_' + obsid + '_bin' + str(tbin_size) + 's_' + str(E1) + 'keV-' + str(E2) + 'keV.pdf'
plt.savefig(parent_folder+'/'+filename,dpi=900)
plt.close()
return phase_bins[:-1],summed_profile
if __name__ == "__main__":
eventfile = '/Volumes/Samsung_T5/NICERsoft_outputs/1034070101_pipe/ni1034070101_nicersoft_bary.evt'
#whole(eventfile,['TIME','PI','PI_FAST'],0.01,[0.20801275,0,0],0.4,21,'show')
#partial_t(eventfile,['TIME','PI','PI_FAST'],1,[0.2081,0,0],0.4,21,0,400,'show')
#partial_E(eventfile,['TIME','PI','PI_FAST'],1,0.05,[0.2081,0,0],0.4,21,0.3,12,'show')
#partial_tE(eventfile,['TIME','PI','PI_FAST'],1,0.05,[0.2081,0,0],0.4,21,0,400,0.3,12,'show')