help='Assigns how many background trials are used in each batch.')
parser.add_option('--years',
dest='years',
type=int,
default=3,
metavar='YEARS',
help='Number of years of data')
opts, args = parser.parse_args()
batch = opts.batch
batchsize = opts.batchsize
years = opts.years
##For this check we'll use the gamma weighting scheme for llh method and injection. We'll add years of data depending on the variable 'years'.
llh59 = data_multi.init59(energy=True, weighting=flux)
llh79 = data_multi.init79(energy=True, weighting=flux)
llh86 = data_multi.init86I(energy=True, weighting=flux)
samples = [llh59, llh79, llh86]
llhmodel = data_multi.multi_init(samples, energy=True)
bckg_trials = PointSourceLLH.background_scrambles(llhmodel,
src_ra,
src_dec,
alpha=0.5,
maxiter=batchsize)
#choose an output dir, and make sure it exists
this_dir = os.path.dirname(os.path.abspath(__file__))
out_dir = misc.ensure_dir(
src_ra = [0.0]
## Now to import my llh model framework. ##
import data_multi
## Like in the background trials, we have to define which llhmodel to use.
##Now, I'll input my injections scheme (same for cut and uncut) and likelihood model (mc varies with injection range). ##
inj = PointSourceInjector(Gamma, sinDec_bandwidth=.05, src_dec=src_dec, seed=0)
if year == '40':
llhmodel = data_multi.init40(energy=True, mode='box')
elif year == '79':
llhmodel = data_multi.init79(energy=True, mode='box')
elif year == '86':
llhmodel = data_multi.init86I(energy=True, mode='box')
elif year == '59':
llhmodel = data_multi.init59(energy=True, mode='box')
#If I change the injection range I'll redefine the _e_range variable in ps_injector_stack.py.
sensitivity = PointSourceLLH.weighted_sensitivity(llhmodel,
src_ra=src_ra,
src_dec=src_dec,
alpha=.5,
beta=.9,
inj=inj,
trials={
'n_inj': [],
'TS': [],
'nsources': [],
'gamma': []
},
src_ra, src_dec, redshift, gamma, flux, lum = params['ra'], params[
'dec'], params['redshift'], params['gamma'], params['flux'], params['lum']
## Time to define my modelweights in a dictionary. ##
modelweights = {'flux': flux, 'redshift': list(np.power(redshift, -2))}
## Now to import my llh model framework. ##
import data_multi
## Like in the background trials, we have to define which llhmodel to use.
if llhweight == 'uniform':
llh79 = data_multi.init79(energy=True)
llh86I = data_multi.init86I(energy=True)
llh59 = data_multi.init59(energy=True)
llh40 = data_multi.init40(energy=True)
else:
llh40 = data_multi.init40(energy=True,
weighting=modelweights['{}'.format(llhweight)])
llh79 = data_multi.init79(energy=True,
weighting=modelweights['{}'.format(llhweight)])
llh86I = data_multi.init86I(energy=True,
weighting=modelweights['{}'.format(llhweight)])
llh59 = data_multi.init59(energy=True,
weighting=modelweights['{}'.format(llhweight)])
#We've loaded in the appropriate llh samples, now let's put them both in the blender (not sure about weighting)
if n == 2:
samples = [llh79, llh86I]
'n_inj': n_inj,
'nsources': np.asarray(nsources),
'TS': np.asarray(TS),
'beta': beta,
'beta_err': beta_err,
'TS_beta': TS_beta,
'gamma': np.asarray(gamma)
}
## Now to import my llh model framework. Both the llhmodel and injector have to be the old version, but the data is all the stuff used by the new version - totally up to date.##
import data_multi
## Like in the background trials, we have to define which llhmodel to use.
llh79 = data_multi.init79(energy=True)
llh86I = data_multi.init86I(energy=True)
llh59 = data_multi.init59(energy=True)
llh40 = data_multi.init40(energy=True)
#We've loaded in the appropriate llh samples, now let's put them both in the blender (not sure about weighting)
samples = [llh40, llh59, llh79, llh86I]
llhmodel = data_multi.multi_init(samples, energy=True)
##Remember, weighted sensitivity requires src dec in radians.#
##Now, I'll input my injection weighting scheme from the commandline. APPARENTLY, I need these as radians, not sin(dec).##
#Also, I need to clip these just before they hit the pole - otherwise I'm gonna get out of bounds errors.
limit = np.round(np.pi / 2, 7)
#DONT change the rounding on limit - I chose it specifically because it rounds down.
src_dec = np.clip(np.arcsin(np.linspace(-1, 1, 21)), -limit, limit)
def plot_error(year):
#The following currently devoted to making energy and angular error plots for a year of data.
# init likelihood class
if year == 40:
llh = data_multi.init40(energy=True)
mc = cache.load(filename_pickle + "IC40/mc.pickle")
extra = cache.load(filename_pickle + "IC40/dpsi.pickle")
if year == 59:
llh = data_multi.init59(energy=True)
mc = cache.load(filename_pickle + "IC59/mc.pickle")
extra = cache.load(filename_pickle + "IC59/dpsi.pickle")
if year == 79:
llh = data_multi.init79(energy=True)
mc = cache.load(filename_pickle + "IC79/mc.pickle")
extra = cache.load(filename_pickle + "IC79/dpsi.pickle")
elif year == 86:
llh = data_multi.init86I(energy=True)
mc = cache.load(filename_pickle + "IC86I/mc.pickle")
extra = cache.load(filename_pickle + "IC86I/dpsi.pickle")
dpsi = extra['dpsi']
print(llh)
# datatest
#Currently don't need to remake these plots. but DONT DELETE
colors = ['b', 'g', 'y', 'r']
gamma = np.linspace(1., 2.7, 4)
# fig_energy, (ax1, ax2) = plt.subplots(ncols=2)
# ax1.hist([llh.exp["logE"]] + [mc["logE"] for i in gamma],
# weights=[np.ones(len(llh.exp))]
# + [mc["ow"] * mc["trueE"]**(-g) for g in gamma],
# label=["Pseudo-Data"] + [r"$\gamma={0:.1f}$".format(g) for g in gamma], color= ['k'] + [colors[g] for g in range(len(gamma))],
# histtype="step", bins=100, log=True, normed=True, cumulative=-1)
# ax1.legend(loc="best")
# ax1.set_title("Reconstructed Energy - IC{}".format(str(year)))
# ax1.set_xlabel("logE")
# ax1.set_ylabel("Relative Abundance")
# ax1.hist([llh.exp["logE"]] + [mc["logE"] for i in gamma],
# weights=[np.ones(len(llh.exp))]
# + [mc["ow"] * mc["trueE"]**(-g) for g in gamma],
# label=["Data"] + [r"$\gamma={0:.1f}$".format(g) for g in gamma], color= ['k'] + [colors[g] for g in range(len(gamma))],
# histtype="step", bins=100, log=True, normed=True, cumulative=-1)
# ax2.set_title("Zoomed In")
# ax2.set_xlabel("logE")
# ax2.set_xlim(4,10)
# ax2.set_ylim(1e-5,1)
# ax2.hist([llh.exp["logE"]] + [mc["logE"] for i in gamma],
# weights=[np.ones(len(llh.exp))]
# + [mc["ow"] * mc["trueE"]**(-g) for g in gamma],
# label=["Pseudo-Data"] + [r"$\gamma={0:.1f}$".format(g) for g in gamma], color= ['k'] + [colors[g] for g in range(len(gamma))],
# histtype="step", bins=100, log=True, normed=True, cumulative=-1)
# fig_energy.savefig(filename_plots + 'energy_hists_IC{}.pdf'.format(str(year)))
fig_angular_error, (ax1, ax2) = plt.subplots(ncols=2, figsize=(10, 5))
dec = np.arcsin(mc["sinDec"])
angdist = np.degrees(dpsi)
ax1.hist([np.log10(np.degrees(mc["sigma"])) for i in gamma],
label=[r"$\sigma$ - $\gamma={0:.1f}$".format(g) for g in gamma],
linestyle='dashed',
weights=[mc["ow"] * mc["trueE"]**(-g) for g in gamma],
color=[colors[g] for g in range(len(gamma))],
histtype="step",
bins=100,
normed=True)
ax1.hist(
[np.log10(angdist) for i in gamma],
label=[r"$\Delta \psi$ - $\gamma={0:.1f}$".format(g) for g in gamma],
weights=[mc["ow"] * mc["trueE"]**(-g) for g in gamma],
linestyle='solid',
color=[colors[g] for g in range(len(gamma))],
histtype="step",
bins=100,
normed=True)
ax1.set_title("Reco MC Angular Error Check - IC{}".format(str(year)))
ax1.set_xlabel(r"log$\sigma_{ang}$ (degrees)")
ax1.set_ylabel("Relative Abundance")
ax1.set_ylim(0, 1.5)
ax2.hist([(np.degrees(mc["sigma"])) for i in gamma],
label=[r"$\sigma$ - $\gamma={0:.1f}$".format(g) for g in gamma],
linestyle='dashed',
weights=[mc["ow"] * mc["trueE"]**(-g) for g in gamma],
color=[colors[g] for g in range(len(gamma))],
histtype="step",
bins=1000,
normed=True)
ax2.hist(
[(angdist) for i in gamma],
label=[r"$\Delta \psi$ - $\gamma={0:.1f}$".format(g) for g in gamma],
weights=[mc["ow"] * mc["trueE"]**(-g) for g in gamma],
linestyle='solid',
color=[colors[g] for g in range(len(gamma))],
histtype="step",
bins=1000,
normed=True)
ax2.legend(loc="upper right")
ax2.set_xlim(0, 5)
ax2.set_ylim(0, 3.5)
ax2.set_xlabel(r"$\sigma_{ang}$ (degrees)")
fig_angular_error.savefig(filename_plots +
'angular_error_hists_IC{}.pdf'.format(str(year)))