def correct_off_angle(data, origin=None):
import ctapipe.utils.linalg as linalg
origin = origin or linalg.set_phi_theta(90 * u.deg, 20 * u.deg)
reco_dirs = linalg.set_phi_theta(data["phi"] * u.deg.to(u.rad),
data["theta"] * u.deg.to(u.rad)).T
off_angles = np.arccos(np.clip(np.dot(reco_dirs, origin), -1., 1.)) * u.rad
data["off_angle"] = off_angles.to(u.deg)
def correct_off_angle(data, origin=None):
import ctapipe.utils.linalg as linalg
origin = origin or linalg.set_phi_theta(90 * u.deg, 20 * u.deg)
reco_dirs = linalg.set_phi_theta(data["phi"] * u.deg.to(u.rad),
data["theta"] * u.deg.to(u.rad)).T
off_angles = np.arccos(np.clip(np.dot(reco_dirs, origin), -1., 1.)) * u.rad
data["off_angle"] = off_angles.to(u.deg)
def guess_pix_direction(pix_x,
pix_y,
tel_phi,
tel_theta,
tel_foclen,
camera_rotation=0 * u.degree):
'''
TODO replace with proper implementation
calculates the direction vector of corresponding to a
(x,y) position on the camera
beta is the pixel's angular distance to the centre
according to beta / tel_view = r / maxR
alpha is the polar angle between the y-axis and the pixel
to find the direction the pixel is looking at:
- the pixel direction is set to the telescope direction
- offset by beta towards up
- rotated around the telescope direction by the angle alpha
Parameters
-----------
pix_x, pix_y : ndarray
lists of x and y positions on the camera
tel_phi, tel_theta: astropy quantities
two angles that describe the orientation of the telescope
tel_foclen : astropy quantity
focal length of the telescope
camera_rotation : astropy quantity
rotation of the camera frame inside of the telescope
Returns
-------
pix_dirs : ndarray
shape (n,3) list of "direction vectors"
corresponding to a position on the camera
'''
pix_alpha = np.arctan2(pix_x, pix_y)
pix_rho = (pix_x**2 + pix_y**2)**.5
pix_beta = pix_rho / tel_foclen * u.rad
tel_dir = linalg.set_phi_theta(tel_phi, tel_theta)
pix_dirs = []
for a, b in zip(pix_alpha, pix_beta):
pix_dir = linalg.set_phi_theta(tel_phi, tel_theta + b)
pix_dir = linalg.rotate_around_axis(pix_dir, tel_dir,
(a - camera_rotation))
pix_dirs.append(pix_dir * u.dimless)
return pix_dirs
def guess_pix_direction(pix_x, pix_y, tel_phi, tel_theta, tel_foclen,
camera_rotation=0 * u.degree):
'''
TODO replace with proper implementation
calculates the direction vector of corresponding to a
(x,y) position on the camera
beta is the pixel's angular distance to the centre
according to beta / tel_view = r / maxR
alpha is the polar angle between the y-axis and the pixel
to find the direction the pixel is looking at:
- the pixel direction is set to the telescope direction
- offset by beta towards up
- rotated around the telescope direction by the angle alpha
Parameters
-----------
pix_x, pix_y : ndarray
lists of x and y positions on the camera
tel_phi, tel_theta: astropy quantities
two angles that describe the orientation of the telescope
tel_foclen : astropy quantity
focal length of the telescope
camera_rotation : astropy quantity
rotation of the camera frame inside of the telescope
Returns
-------
pix_dirs : ndarray
shape (n,3) list of "direction vectors"
corresponding to a position on the camera
'''
pix_alpha = np.arctan2(pix_x, pix_y)
pix_rho = (pix_x ** 2 + pix_y ** 2) ** .5
pix_beta = pix_rho / tel_foclen * u.rad
tel_dir = linalg.set_phi_theta(tel_phi, tel_theta)
pix_dirs = []
for a, b in zip(pix_alpha, pix_beta):
pix_dir = linalg.set_phi_theta(tel_phi, tel_theta + b)
pix_dir = linalg.rotate_around_axis(pix_dir, tel_dir,
(a - camera_rotation))
pix_dirs.append(pix_dir * u.dimless)
return pix_dirs
def main():
# your favourite units here
energy_unit = u.TeV
angle_unit = u.deg
dist_unit = u.m
parser = make_argparser()
parser.add_argument('-o', '--outfile', type=str,
help="if given, write output file with reconstruction results")
parser.add_argument('--plot_c', action='store_true',
help="plot camera-wise displays")
group = parser.add_mutually_exclusive_group()
group.add_argument('--proton', action='store_true',
help="do protons instead of gammas")
group.add_argument('--electron', action='store_true',
help="do electrons instead of gammas")
args = parser.parse_args()
if args.infile_list:
filenamelist = []
for f in args.infile_list:
filenamelist += glob("{}/{}".format(args.indir, f))
elif args.proton:
filenamelist = glob("{}/proton/*gz".format(args.indir))
channel = "proton"
elif args.electron:
filenamelist = glob("{}/electron/*gz".format(args.indir))
channel = "electron"
elif args.gamma:
filenamelist = glob("{}/gamma/*gz".format(args.indir))
channel = "gamma"
else:
raise ValueError("don't know which input to use...")
filenamelist.sort()
if not filenamelist:
print("no files found; check indir: {}".format(args.indir))
exit(-1)
else:
print("found {} files".format(len(filenamelist)))
tel_phi = {}
tel_theta = {}
# keeping track of events and where they were rejected
Eventcutflow = CutFlow("EventCutFlow")
Imagecutflow = CutFlow("ImageCutFlow")
# takes care of image cleaning
cleaner = ImageCleaner(mode=args.mode, cutflow=Imagecutflow,
wavelet_options=args.raw,
skip_edge_events=args.skip_edge_events, island_cleaning=True)
# the class that does the shower reconstruction
shower_reco = HillasReconstructor()
shower_max_estimator = ShowerMaxEstimator("paranal")
preper = EventPreparer(cleaner=cleaner,
hillas_parameters=hillas_parameters, shower_reco=shower_reco,
event_cutflow=Eventcutflow, image_cutflow=Imagecutflow,
# event/image cuts:
allowed_cam_ids=[], # means: all
min_ntel=3,
min_charge=args.min_charge,
min_pixel=3)
# a signal handler to abort the event loop but still do the post-processing
signal_handler = SignalHandler()
signal.signal(signal.SIGINT, signal_handler)
try:
# this class defines the reconstruction parameters to keep track of
class RecoEvent(tb.IsDescription):
NTels_trigg = tb.Int16Col(dflt=1, pos=0)
NTels_clean = tb.Int16Col(dflt=1, pos=1)
EnMC = tb.Float32Col(dflt=1, pos=2)
xi = tb.Float32Col(dflt=1, pos=3)
DeltaR = tb.Float32Col(dflt=1, pos=4)
ErrEstPos = tb.Float32Col(dflt=1, pos=5)
ErrEstDir = tb.Float32Col(dflt=1, pos=6)
h_max = tb.Float32Col(dflt=1, pos=7)
reco_outfile = tb.open_file(
args.outfile, mode="w",
# if we don't want to write the event list to disk, need to add more arguments
**({} if args.store else {"driver": "H5FD_CORE",
"driver_core_backing_store": False}))
reco_table = reco_outfile.create_table("/", "reco_event", RecoEvent)
reco_event = reco_table.row
except:
reco_event = RecoEvent()
print("no pytables installed?")
# ## ####### ####### ########
# ## ## ## ## ## ## ##
# ## ## ## ## ## ## ##
# ## ## ## ## ## ########
# ## ## ## ## ## ##
# ## ## ## ## ## ##
# ######## ####### ####### ##
cam_id_map = {}
# define here which telescopes to loop over
allowed_tels = None
# allowed_tels = prod3b_tel_ids("L+F+D")
for i, filename in enumerate(filenamelist[:args.last]):
print("file: {i} filename = {filename}".format(i=i, filename=filename))
source = hessio_event_source(filename,
allowed_tels=allowed_tels,
max_events=args.max_events)
# loop that cleans and parametrises the images and performs the reconstruction
for (event, hillas_dict, n_tels,
tot_signal, max_signal, pos_fit, dir_fit, h_max,
err_est_pos, err_est_dir) in preper.prepare_event(source):
shower = event.mc
org_alt = u.Quantity(shower.alt).to(u.deg)
org_az = u.Quantity(shower.az).to(u.deg)
if org_az > 180 * u.deg:
org_az -= 360 * u.deg
org_the = alt_to_theta(org_alt)
org_phi = az_to_phi(org_az)
if org_phi > 180 * u.deg:
org_phi -= 360 * u.deg
if org_phi < -180 * u.deg:
org_phi += 360 * u.deg
shower_org = linalg.set_phi_theta(org_phi, org_the)
shower_core = convert_astropy_array([shower.core_x, shower.core_y])
xi = linalg.angle(dir_fit, shower_org).to(angle_unit)
diff = linalg.length(pos_fit[:2] - shower_core)
# print some performance
print()
print("xi = {:4.3f}".format(xi))
print("pos = {:4.3f}".format(diff))
print("h_max reco: {:4.3f}".format(h_max.to(u.km)))
print("err_est_dir: {:4.3f}".format(err_est_dir.to(angle_unit)))
print("err_est_pos: {:4.3f}".format(err_est_pos))
try:
# store the reconstruction data in the PyTable
reco_event["NTels_trigg"] = n_tels["tot"]
reco_event["NTels_clean"] = len(shower_reco.circles)
reco_event["EnMC"] = event.mc.energy / energy_unit
reco_event["xi"] = xi / angle_unit
reco_event["DeltaR"] = diff / dist_unit
reco_event["ErrEstPos"] = err_est_pos / dist_unit
reco_event["ErrEstDir"] = err_est_dir / angle_unit
reco_event["h_max"] = h_max / dist_unit
reco_event.append()
reco_table.flush()
print()
print("xi res (68-percentile) = {:4.3f} {}"
.format(np.percentile(reco_table.cols.xi, 68), angle_unit))
print("core res (68-percentile) = {:4.3f} {}"
.format(np.percentile(reco_table.cols.DeltaR, 68), dist_unit))
print("h_max (median) = {:4.3f} {}"
.format(np.percentile(reco_table.cols.h_max, 50), dist_unit))
except NoPyTables:
pass
if args.plot_c:
from mpl_toolkits.mplot3d import Axes3D
fig = plt.figure()
ax = fig.gca(projection='3d')
for c in shower_reco.circles.values():
points = [c.pos + t * c.a * u.km for t in np.linspace(0, 15, 3)]
ax.plot(*np.array(points).T, linewidth=np.sqrt(c.weight) / 10)
ax.scatter(*c.pos[:, None].value, s=np.sqrt(c.weight))
plt.xlabel("x")
plt.ylabel("y")
plt.pause(.1)
# this plots
# • the MC shower core
# • the reconstructed shower core
# • the used telescopes
# • and the trace of the Hillas plane on the ground
plt.figure()
for tel_id, c in shower_reco.circles.items():
plt.scatter(c.pos[0], c.pos[1], s=np.sqrt(c.weight))
plt.gca().annotate(tel_id, (c.pos[0].value, c.pos[1].value))
plt.plot([c.pos[0].value-500*c.norm[1], c.pos[0].value+500*c.norm[1]],
[c.pos[1].value+500*c.norm[0], c.pos[1].value-500*c.norm[0]],
linewidth=np.sqrt(c.weight)/10)
plt.scatter(*pos_fit[:2], c="black", marker="*", label="fitted")
plt.scatter(*shower_core[:2], c="black", marker="P", label="MC")
plt.legend()
plt.xlabel("x")
plt.ylabel("y")
plt.xlim(-1400, 1400)
plt.ylim(-1400, 1400)
plt.show()
if signal_handler.stop: break
if signal_handler.stop: break
print("\n" + "="*35 + "\n")
print("xi res (68-percentile) = {:4.3f} {}"
.format(np.percentile(reco_table.cols.xi, 68), angle_unit))
print("core res (68-percentile) = {:4.3f} {}"
.format(np.percentile(reco_table.cols.DeltaR, 68), dist_unit))
print("h_max (median) = {:4.3f} {}"
.format(np.percentile(reco_table.cols.h_max, 50), dist_unit))
# print the cutflows for telescopes and camera images
print("\n\n")
Eventcutflow("min2Tels trig")
print()
Imagecutflow(sort_column=1)
# if we don't want to plot anything, we can exit now
if not args.plot:
return
# ######## ## ####### ######## ######
# ## ## ## ## ## ## ## ##
# ## ## ## ## ## ## ##
# ######## ## ## ## ## ######
# ## ## ## ## ## ##
# ## ## ## ## ## ## ##
# ## ######## ####### ## ######
plt.figure()
plt.hist(reco_table.cols.h_max, bins=np.linspace(000, 15000, 51, True))
plt.title(channel)
plt.xlabel("h_max reco")
plt.pause(.1)
figure = plt.figure()
xi_edges = np.linspace(0, 5, 20)
plt.hist(reco_table.cols.xi, bins=xi_edges, log=True)
plt.xlabel(r"$\xi$ / deg")
if args.write:
save_fig('{}/reco_xi_{}'.format(args.plots_dir, args.mode))
plt.pause(.1)
plt.figure()
plt.hist(reco_table.cols.ErrEstDir[:],
bins=np.linspace(0, 20, 50))
plt.title(channel)
plt.xlabel("beta")
plt.pause(.1)
plt.figure()
plt.hist(np.log10(reco_table.cols.xi[:] / reco_table.cols.ErrEstDir[:]), bins=50)
plt.title(channel)
plt.xlabel("log_10(xi / beta)")
plt.pause(.1)
# convert the xi-list into a dict with the number of used telescopes as keys
xi_vs_tel = {}
for xi, ntel in zip(reco_table.cols.xi, reco_table.cols.NTels_clean):
if ntel not in xi_vs_tel:
xi_vs_tel[ntel] = [xi]
else:
xi_vs_tel[ntel].append(xi)
print(args.mode)
for ntel, xis in sorted(xi_vs_tel.items()):
print("NTel: {} -- median xi: {}".format(ntel, np.median(xis)))
# print("histogram:", np.histogram(xis, bins=xi_edges))
# create a list of energy bin-edges and -centres for violin plots
Energy_edges = np.linspace(2, 8, 13)
Energy_centres = (Energy_edges[1:]+Energy_edges[:-1])/2.
# convert the xi-list in to an energy-binned dict with the bin centre as keys
xi_vs_energy = {}
for en, xi in zip(reco_table.cols.EnMC, reco_table.cols.xi):
# get the bin number this event belongs into
sbin = np.digitize(np.log10(en), Energy_edges)-1
# the central value of the bin is the key for the dictionary
if Energy_centres[sbin] not in xi_vs_energy:
xi_vs_energy[Energy_centres[sbin]] = [xi]
else:
xi_vs_energy[Energy_centres[sbin]] += [xi]
# plotting the angular error as violin plots with binning in
# number of telescopes and shower energy
figure = plt.figure()
plt.subplot(211)
plt.violinplot([np.log10(a) for a in xi_vs_tel.values()],
[a for a in xi_vs_tel.keys()],
points=60, widths=.75, showextrema=False, showmedians=True)
plt.xlabel("Number of Telescopes")
plt.ylabel(r"log($\xi$ / deg)")
plt.ylim(-3, 2)
plt.grid()
plt.subplot(212)
plt.violinplot([np.log10(a) for a in xi_vs_energy.values()],
[a for a in xi_vs_energy.keys()],
points=60, widths=(Energy_edges[1] - Energy_edges[0]) / 1.5,
showextrema=False, showmedians=True)
plt.xlabel(r"log(Energy / GeV)")
plt.ylabel(r"log($\xi$ / deg)")
plt.ylim(-3, 2)
plt.grid()
plt.tight_layout()
if args.write:
save_fig('{}/reco_xi_vs_E_NTel_{}'.format(args.plots_dir, args.mode))
plt.pause(.1)
# convert the diffs-list into a dict with the number of used telescopes as keys
diff_vs_tel = {}
for diff, ntel in zip(reco_table.cols.DeltaR, reco_table.cols.NTels_clean):
if ntel not in diff_vs_tel:
diff_vs_tel[ntel] = [diff]
else:
diff_vs_tel[ntel].append(diff)
# convert the diffs-list in to an energy-binned dict with the bin centre as keys
diff_vs_energy = {}
for en, diff in zip(reco_table.cols.EnMC, reco_table.cols.DeltaR):
# get the bin number this event belongs into
sbin = np.digitize(np.log10(en), Energy_edges) - 1
# the central value of the bin is the key for the dictionary
if Energy_centres[sbin] not in diff_vs_energy:
diff_vs_energy[Energy_centres[sbin]] = [diff]
else:
diff_vs_energy[Energy_centres[sbin]] += [diff]
# plotting the core position error as violin plots with binning in
# number of telescopes an shower energy
plt.figure()
plt.subplot(211)
plt.violinplot([np.log10(a) for a in diff_vs_tel.values()],
[a for a in diff_vs_tel.keys()],
points=60, widths=.75, showextrema=False, showmedians=True)
plt.xlabel("Number of Telescopes")
plt.ylabel(r"log($\Delta R$ / m)")
plt.grid()
plt.subplot(212)
plt.violinplot([np.log10(a) for a in diff_vs_energy.values()],
[a for a in diff_vs_energy.keys()],
points=60, widths=(Energy_edges[1] - Energy_edges[0]) / 1.5,
showextrema=False, showmedians=True)
plt.xlabel(r"log(Energy / GeV)")
plt.ylabel(r"log($\Delta R$ / m)")
plt.grid()
plt.tight_layout()
if args.write:
save_fig('{}/reco_dist_vs_E_NTel_{}'.format(args.plots_dir, args.mode))
plt.show()
def main():
# your favourite units here
energy_unit = u.TeV
angle_unit = u.deg
dist_unit = u.m
agree_threshold = .5
min_tel = 3
parser = make_argparser()
parser.add_argument('--classifier',
type=str,
default=expandvars(
"$CTA_SOFT/tino_cta/data/classifier_pickle/"
"classifier_{mode}_{cam_id}_{classifier}.pkl"))
parser.add_argument('--regressor',
type=str,
default=expandvars(
"$CTA_SOFT/tino_cta/data/classifier_pickle/"
"regressor_{mode}_{cam_id}_{regressor}.pkl"))
parser.add_argument('-o',
'--outfile',
type=str,
default="",
help="location to write the classified events to.")
parser.add_argument('--wave_dir',
type=str,
default=None,
help="directory where to find mr_filter. "
"if not set look in $PATH")
parser.add_argument(
'--wave_temp_dir',
type=str,
default='/dev/shm/',
help="directory where mr_filter to store the temporary fits "
"files")
group = parser.add_mutually_exclusive_group()
group.add_argument('--proton',
action='store_true',
help="do protons instead of gammas")
group.add_argument('--electron',
action='store_true',
help="do electrons instead of gammas")
args = parser.parse_args()
if args.infile_list:
filenamelist = []
for f in args.infile_list:
filenamelist += glob("{}/{}".format(args.indir, f))
filenamelist.sort()
elif args.proton:
filenamelist = sorted(glob("{}/proton/*gz".format(args.indir)))
elif args.electron:
filenamelist = glob("{}/electron/*gz".format(args.indir))
channel = "electron"
else:
filenamelist = sorted(glob("{}/gamma/*gz".format(args.indir)))
if not filenamelist:
print("no files found; check indir: {}".format(args.indir))
exit(-1)
# keeping track of events and where they were rejected
Eventcutflow = CutFlow("EventCutFlow")
Imagecutflow = CutFlow("ImageCutFlow")
# takes care of image cleaning
cleaner = ImageCleaner(mode=args.mode,
cutflow=Imagecutflow,
wavelet_options=args.raw,
tmp_files_directory=args.wave_temp_dir,
skip_edge_events=False,
island_cleaning=True)
# the class that does the shower reconstruction
shower_reco = HillasReconstructor()
preper = EventPreparer(
cleaner=cleaner,
hillas_parameters=hillas_parameters,
shower_reco=shower_reco,
event_cutflow=Eventcutflow,
image_cutflow=Imagecutflow,
# event/image cuts:
allowed_cam_ids=[],
min_ntel=2,
min_charge=args.min_charge,
min_pixel=3)
# wrapper for the scikit-learn classifier
classifier = EventClassifier.load(args.classifier.format(
**{
"mode": args.mode,
"wave_args": "mixed",
"classifier": 'RandomForestClassifier',
"cam_id": "{cam_id}"
}),
cam_id_list=args.cam_ids)
# wrapper for the scikit-learn regressor
regressor = EnergyRegressor.load(args.regressor.format(
**{
"mode": args.mode,
"wave_args": "mixed",
"regressor": "RandomForestRegressor",
"cam_id": "{cam_id}"
}),
cam_id_list=args.cam_ids)
ClassifierFeatures = namedtuple(
"ClassifierFeatures",
("impact_dist", "sum_signal_evt", "max_signal_cam", "sum_signal_cam",
"N_LST", "N_MST", "N_SST", "width", "length", "skewness", "kurtosis",
"h_max", "err_est_pos", "err_est_dir"))
EnergyFeatures = namedtuple(
"EnergyFeatures",
("impact_dist", "sum_signal_evt", "max_signal_cam", "sum_signal_cam",
"N_LST", "N_MST", "N_SST", "width", "length", "skewness", "kurtosis",
"h_max", "err_est_pos", "err_est_dir"))
# catch ctr-c signal to exit current loop and still display results
signal_handler = SignalHandler()
signal.signal(signal.SIGINT, signal_handler)
# this class defines the reconstruction parameters to keep track of
class RecoEvent(tb.IsDescription):
Run_ID = tb.Int16Col(dflt=-1, pos=0)
Event_ID = tb.Int16Col(dflt=-1, pos=1)
NTels_trig = tb.Int16Col(dflt=0, pos=0)
NTels_reco = tb.Int16Col(dflt=0, pos=1)
NTels_reco_lst = tb.Int16Col(dflt=0, pos=2)
NTels_reco_mst = tb.Int16Col(dflt=0, pos=3)
NTels_reco_sst = tb.Int16Col(dflt=0, pos=4)
MC_Energy = tb.Float32Col(dflt=np.nan, pos=5)
reco_Energy = tb.Float32Col(dflt=np.nan, pos=6)
reco_phi = tb.Float32Col(dflt=np.nan, pos=7)
reco_theta = tb.Float32Col(dflt=np.nan, pos=8)
off_angle = tb.Float32Col(dflt=np.nan, pos=9)
xi = tb.Float32Col(dflt=np.nan, pos=10)
DeltaR = tb.Float32Col(dflt=np.nan, pos=11)
ErrEstPos = tb.Float32Col(dflt=np.nan, pos=12)
ErrEstDir = tb.Float32Col(dflt=np.nan, pos=13)
gammaness = tb.Float32Col(dflt=np.nan, pos=14)
success = tb.BoolCol(dflt=False, pos=15)
channel = "gamma" if "gamma" in " ".join(filenamelist) else "proton"
reco_outfile = tb.open_file(
mode="w",
# if no outfile name is given (i.e. don't to write the event list to disk),
# need specify two "driver" arguments
**({
"filename": args.outfile
} if args.outfile else {
"filename": "no_outfile.h5",
"driver": "H5FD_CORE",
"driver_core_backing_store": False
}))
reco_table = reco_outfile.create_table("/", "reco_events", RecoEvent)
reco_event = reco_table.row
allowed_tels = None # all telescopes
allowed_tels = prod3b_tel_ids("L+N+D")
for i, filename in enumerate(filenamelist[:args.last]):
# print(f"file: {i} filename = {filename}")
source = hessio_event_source(filename,
allowed_tels=allowed_tels,
max_events=args.max_events)
# loop that cleans and parametrises the images and performs the reconstruction
for (event, hillas_dict, n_tels, tot_signal, max_signals, pos_fit,
dir_fit, h_max, err_est_pos,
err_est_dir) in preper.prepare_event(source, True):
# now prepare the features for the classifier
cls_features_evt = {}
reg_features_evt = {}
if hillas_dict is not None:
for tel_id in hillas_dict.keys():
Imagecutflow.count("pre-features")
tel_pos = np.array(event.inst.tel_pos[tel_id][:2]) * u.m
moments = hillas_dict[tel_id]
impact_dist = linalg.length(tel_pos - pos_fit)
cls_features_tel = ClassifierFeatures(
impact_dist=impact_dist / u.m,
sum_signal_evt=tot_signal,
max_signal_cam=max_signals[tel_id],
sum_signal_cam=moments.size,
N_LST=n_tels["LST"],
N_MST=n_tels["MST"],
N_SST=n_tels["SST"],
width=moments.width / u.m,
length=moments.length / u.m,
skewness=moments.skewness,
kurtosis=moments.kurtosis,
h_max=h_max / u.m,
err_est_pos=err_est_pos / u.m,
err_est_dir=err_est_dir / u.deg)
reg_features_tel = EnergyFeatures(
impact_dist=impact_dist / u.m,
sum_signal_evt=tot_signal,
max_signal_cam=max_signals[tel_id],
sum_signal_cam=moments.size,
N_LST=n_tels["LST"],
N_MST=n_tels["MST"],
N_SST=n_tels["SST"],
width=moments.width / u.m,
length=moments.length / u.m,
skewness=moments.skewness,
kurtosis=moments.kurtosis,
h_max=h_max / u.m,
err_est_pos=err_est_pos / u.m,
err_est_dir=err_est_dir / u.deg)
if np.isnan(cls_features_tel).any() or np.isnan(
reg_features_tel).any():
continue
Imagecutflow.count("features nan")
cam_id = event.inst.subarray.tel[tel_id].camera.cam_id
try:
reg_features_evt[cam_id] += [reg_features_tel]
cls_features_evt[cam_id] += [cls_features_tel]
except KeyError:
reg_features_evt[cam_id] = [reg_features_tel]
cls_features_evt[cam_id] = [cls_features_tel]
if cls_features_evt and reg_features_evt:
predict_energ = regressor.predict_by_event([reg_features_evt
])["mean"][0]
predict_proba = classifier.predict_proba_by_event(
[cls_features_evt])
gammaness = predict_proba[0, 0]
try:
# the MC direction of origin of the simulated particle
shower = event.mc
shower_core = np.array(
[shower.core_x / u.m, shower.core_y / u.m]) * u.m
shower_org = linalg.set_phi_theta(az_to_phi(shower.az),
alt_to_theta(shower.alt))
# and how the reconstructed direction compares to that
xi = linalg.angle(dir_fit, shower_org)
DeltaR = linalg.length(pos_fit[:2] - shower_core)
except Exception:
# naked exception catch, because I'm not sure where
# it would break in non-MC files
xi = np.nan
DeltaR = np.nan
phi, theta = linalg.get_phi_theta(dir_fit)
phi = (phi if phi > 0 else phi + 360 * u.deg)
# TODO: replace with actual array pointing direction
array_pointing = linalg.set_phi_theta(0 * u.deg, 20. * u.deg)
# angular offset between the reconstructed direction and the array
# pointing
off_angle = linalg.angle(dir_fit, array_pointing)
reco_event["NTels_trig"] = len(event.dl0.tels_with_data)
reco_event["NTels_reco"] = len(hillas_dict)
reco_event["NTels_reco_lst"] = n_tels["LST"]
reco_event["NTels_reco_mst"] = n_tels["MST"]
reco_event["NTels_reco_sst"] = n_tels["SST"]
reco_event["reco_Energy"] = predict_energ.to(energy_unit).value
reco_event["reco_phi"] = phi / angle_unit
reco_event["reco_theta"] = theta / angle_unit
reco_event["off_angle"] = off_angle / angle_unit
reco_event["xi"] = xi / angle_unit
reco_event["DeltaR"] = DeltaR / dist_unit
reco_event["ErrEstPos"] = err_est_pos / dist_unit
reco_event["ErrEstDir"] = err_est_dir / angle_unit
reco_event["gammaness"] = gammaness
reco_event["success"] = True
else:
reco_event["success"] = False
# save basic event infos
reco_event["MC_Energy"] = event.mc.energy.to(energy_unit).value
reco_event["Event_ID"] = event.r1.event_id
reco_event["Run_ID"] = event.r1.run_id
reco_table.flush()
reco_event.append()
if signal_handler.stop:
break
if signal_handler.stop:
break
# make sure everything gets written out nicely
reco_table.flush()
try:
print()
Eventcutflow()
print()
Imagecutflow()
# do some simple event selection
# and print the corresponding selection efficiency
N_selected = len([
x for x in reco_table.where(
"""(NTels_reco > min_tel) & (gammaness > agree_threshold)""")
])
N_total = len(reco_table)
print("\nfraction selected events:")
print("{} / {} = {} %".format(N_selected, N_total,
N_selected / N_total * 100))
except ZeroDivisionError:
pass
print("\nlength filenamelist:", len(filenamelist[:args.last]))
# do some plotting if so desired
if args.plot:
gammaness = [x['gammaness'] for x in reco_table]
NTels_rec = [x['NTels_reco'] for x in reco_table]
NTel_bins = np.arange(np.min(NTels_rec), np.max(NTels_rec) + 2) - .5
NTels_rec_lst = [x['NTels_reco_lst'] for x in reco_table]
NTels_rec_mst = [x['NTels_reco_mst'] for x in reco_table]
NTels_rec_sst = [x['NTels_reco_sst'] for x in reco_table]
reco_energy = np.array([x['reco_Energy'] for x in reco_table])
mc_energy = np.array([x['MC_Energy'] for x in reco_table])
fig = plt.figure(figsize=(15, 5))
plt.suptitle(" ** ".join(
[args.mode, "protons" if args.proton else "gamma"]))
plt.subplots_adjust(left=0.05, right=0.97, hspace=0.39, wspace=0.2)
ax = plt.subplot(131)
histo = np.histogram2d(NTels_rec,
gammaness,
bins=(NTel_bins, np.linspace(0, 1, 11)))[0].T
histo_normed = histo / histo.max(axis=0)
im = ax.imshow(
histo_normed,
interpolation='none',
origin='lower',
aspect='auto',
# extent=(*NTel_bins[[0, -1]], 0, 1),
cmap=plt.cm.inferno)
ax.set_xlabel("NTels")
ax.set_ylabel("drifted gammaness")
plt.title("Total Number of Telescopes")
# next subplot
ax = plt.subplot(132)
histo = np.histogram2d(NTels_rec_sst,
gammaness,
bins=(NTel_bins, np.linspace(0, 1, 11)))[0].T
histo_normed = histo / histo.max(axis=0)
im = ax.imshow(
histo_normed,
interpolation='none',
origin='lower',
aspect='auto',
# extent=(*NTel_bins[[0, -1]], 0, 1),
cmap=plt.cm.inferno)
ax.set_xlabel("NTels")
plt.setp(ax.get_yticklabels(), visible=False)
plt.title("Number of SSTs")
# next subplot
ax = plt.subplot(133)
histo = np.histogram2d(NTels_rec_mst,
gammaness,
bins=(NTel_bins, np.linspace(0, 1, 11)))[0].T
histo_normed = histo / histo.max(axis=0)
im = ax.imshow(
histo_normed,
interpolation='none',
origin='lower',
aspect='auto',
# extent=(*NTel_bins[[0, -1]], 0, 1),
cmap=plt.cm.inferno)
cb = fig.colorbar(im, ax=ax)
ax.set_xlabel("NTels")
plt.setp(ax.get_yticklabels(), visible=False)
plt.title("Number of MSTs")
plt.subplots_adjust(wspace=0.05)
# plot the energy migration matrix
plt.figure()
plt.hist2d(np.log10(reco_energy),
np.log10(mc_energy),
bins=20,
cmap=plt.cm.inferno)
plt.xlabel("E_MC / TeV")
plt.ylabel("E_rec / TeV")
plt.colorbar()
plt.show()
def main():
# your favourite units here
energy_unit = u.TeV
angle_unit = u.deg
dist_unit = u.m
parser = make_argparser()
parser.add_argument(
'-o',
'--outfile',
type=str,
help="if given, write output file with reconstruction results")
parser.add_argument('--plot_c',
action='store_true',
help="plot camera-wise displays")
group = parser.add_mutually_exclusive_group()
group.add_argument('--proton',
action='store_true',
help="do protons instead of gammas")
group.add_argument('--electron',
action='store_true',
help="do electrons instead of gammas")
args = parser.parse_args()
if args.infile_list:
filenamelist = []
for f in args.infile_list:
filenamelist += glob("{}/{}".format(args.indir, f))
elif args.proton:
filenamelist = glob("{}/proton/*gz".format(args.indir))
channel = "proton"
elif args.electron:
filenamelist = glob("{}/electron/*gz".format(args.indir))
channel = "electron"
elif args.gamma:
filenamelist = glob("{}/gamma/*gz".format(args.indir))
channel = "gamma"
else:
raise ValueError("don't know which input to use...")
filenamelist.sort()
if not filenamelist:
print("no files found; check indir: {}".format(args.indir))
exit(-1)
else:
print("found {} files".format(len(filenamelist)))
tel_phi = {}
tel_theta = {}
# keeping track of events and where they were rejected
Eventcutflow = CutFlow("EventCutFlow")
Imagecutflow = CutFlow("ImageCutFlow")
# takes care of image cleaning
cleaner = ImageCleaner(mode=args.mode,
cutflow=Imagecutflow,
wavelet_options=args.raw,
skip_edge_events=args.skip_edge_events,
island_cleaning=True)
# the class that does the shower reconstruction
shower_reco = HillasReconstructor()
shower_max_estimator = ShowerMaxEstimator("paranal")
preper = EventPreparer(
cleaner=cleaner,
hillas_parameters=hillas_parameters,
shower_reco=shower_reco,
event_cutflow=Eventcutflow,
image_cutflow=Imagecutflow,
# event/image cuts:
allowed_cam_ids=[], # means: all
min_ntel=3,
min_charge=args.min_charge,
min_pixel=3)
# a signal handler to abort the event loop but still do the post-processing
signal_handler = SignalHandler()
signal.signal(signal.SIGINT, signal_handler)
try:
# this class defines the reconstruction parameters to keep track of
class RecoEvent(tb.IsDescription):
NTels_trigg = tb.Int16Col(dflt=1, pos=0)
NTels_clean = tb.Int16Col(dflt=1, pos=1)
EnMC = tb.Float32Col(dflt=1, pos=2)
xi = tb.Float32Col(dflt=1, pos=3)
DeltaR = tb.Float32Col(dflt=1, pos=4)
ErrEstPos = tb.Float32Col(dflt=1, pos=5)
ErrEstDir = tb.Float32Col(dflt=1, pos=6)
h_max = tb.Float32Col(dflt=1, pos=7)
reco_outfile = tb.open_file(
args.outfile,
mode="w",
# if we don't want to write the event list to disk, need to add more arguments
**({} if args.store else {
"driver": "H5FD_CORE",
"driver_core_backing_store": False
}))
reco_table = reco_outfile.create_table("/", "reco_event", RecoEvent)
reco_event = reco_table.row
except:
reco_event = RecoEvent()
print("no pytables installed?")
# ## ####### ####### ########
# ## ## ## ## ## ## ##
# ## ## ## ## ## ## ##
# ## ## ## ## ## ########
# ## ## ## ## ## ##
# ## ## ## ## ## ##
# ######## ####### ####### ##
cam_id_map = {}
# define here which telescopes to loop over
allowed_tels = None
# allowed_tels = prod3b_tel_ids("L+F+D")
for i, filename in enumerate(filenamelist[:args.last]):
print("file: {i} filename = {filename}".format(i=i, filename=filename))
source = hessio_event_source(filename,
allowed_tels=allowed_tels,
max_events=args.max_events)
# loop that cleans and parametrises the images and performs the reconstruction
for (event, hillas_dict, n_tels, tot_signal, max_signal, pos_fit,
dir_fit, h_max, err_est_pos,
err_est_dir) in preper.prepare_event(source):
shower = event.mc
org_alt = u.Quantity(shower.alt).to(u.deg)
org_az = u.Quantity(shower.az).to(u.deg)
if org_az > 180 * u.deg:
org_az -= 360 * u.deg
org_the = alt_to_theta(org_alt)
org_phi = az_to_phi(org_az)
if org_phi > 180 * u.deg:
org_phi -= 360 * u.deg
if org_phi < -180 * u.deg:
org_phi += 360 * u.deg
shower_org = linalg.set_phi_theta(org_phi, org_the)
shower_core = convert_astropy_array([shower.core_x, shower.core_y])
xi = linalg.angle(dir_fit, shower_org).to(angle_unit)
diff = linalg.length(pos_fit[:2] - shower_core)
# print some performance
print()
print("xi = {:4.3f}".format(xi))
print("pos = {:4.3f}".format(diff))
print("h_max reco: {:4.3f}".format(h_max.to(u.km)))
print("err_est_dir: {:4.3f}".format(err_est_dir.to(angle_unit)))
print("err_est_pos: {:4.3f}".format(err_est_pos))
try:
# store the reconstruction data in the PyTable
reco_event["NTels_trigg"] = n_tels["tot"]
reco_event["NTels_clean"] = len(shower_reco.circles)
reco_event["EnMC"] = event.mc.energy / energy_unit
reco_event["xi"] = xi / angle_unit
reco_event["DeltaR"] = diff / dist_unit
reco_event["ErrEstPos"] = err_est_pos / dist_unit
reco_event["ErrEstDir"] = err_est_dir / angle_unit
reco_event["h_max"] = h_max / dist_unit
reco_event.append()
reco_table.flush()
print()
print("xi res (68-percentile) = {:4.3f} {}".format(
np.percentile(reco_table.cols.xi, 68), angle_unit))
print("core res (68-percentile) = {:4.3f} {}".format(
np.percentile(reco_table.cols.DeltaR, 68), dist_unit))
print("h_max (median) = {:4.3f} {}".format(
np.percentile(reco_table.cols.h_max, 50), dist_unit))
except NoPyTables:
pass
if args.plot_c:
from mpl_toolkits.mplot3d import Axes3D
fig = plt.figure()
ax = fig.gca(projection='3d')
for c in shower_reco.circles.values():
points = [
c.pos + t * c.a * u.km for t in np.linspace(0, 15, 3)
]
ax.plot(*np.array(points).T,
linewidth=np.sqrt(c.weight) / 10)
ax.scatter(*c.pos[:, None].value, s=np.sqrt(c.weight))
plt.xlabel("x")
plt.ylabel("y")
plt.pause(.1)
# this plots
# • the MC shower core
# • the reconstructed shower core
# • the used telescopes
# • and the trace of the Hillas plane on the ground
plt.figure()
for tel_id, c in shower_reco.circles.items():
plt.scatter(c.pos[0], c.pos[1], s=np.sqrt(c.weight))
plt.gca().annotate(tel_id,
(c.pos[0].value, c.pos[1].value))
plt.plot([
c.pos[0].value - 500 * c.norm[1],
c.pos[0].value + 500 * c.norm[1]
], [
c.pos[1].value + 500 * c.norm[0],
c.pos[1].value - 500 * c.norm[0]
],
linewidth=np.sqrt(c.weight) / 10)
plt.scatter(*pos_fit[:2],
c="black",
marker="*",
label="fitted")
plt.scatter(*shower_core[:2],
c="black",
marker="P",
label="MC")
plt.legend()
plt.xlabel("x")
plt.ylabel("y")
plt.xlim(-1400, 1400)
plt.ylim(-1400, 1400)
plt.show()
if signal_handler.stop: break
if signal_handler.stop: break
print("\n" + "=" * 35 + "\n")
print("xi res (68-percentile) = {:4.3f} {}".format(
np.percentile(reco_table.cols.xi, 68), angle_unit))
print("core res (68-percentile) = {:4.3f} {}".format(
np.percentile(reco_table.cols.DeltaR, 68), dist_unit))
print("h_max (median) = {:4.3f} {}".format(
np.percentile(reco_table.cols.h_max, 50), dist_unit))
# print the cutflows for telescopes and camera images
print("\n\n")
Eventcutflow("min2Tels trig")
print()
Imagecutflow(sort_column=1)
# if we don't want to plot anything, we can exit now
if not args.plot:
return
# ######## ## ####### ######## ######
# ## ## ## ## ## ## ## ##
# ## ## ## ## ## ## ##
# ######## ## ## ## ## ######
# ## ## ## ## ## ##
# ## ## ## ## ## ## ##
# ## ######## ####### ## ######
plt.figure()
plt.hist(reco_table.cols.h_max, bins=np.linspace(000, 15000, 51, True))
plt.title(channel)
plt.xlabel("h_max reco")
plt.pause(.1)
figure = plt.figure()
xi_edges = np.linspace(0, 5, 20)
plt.hist(reco_table.cols.xi, bins=xi_edges, log=True)
plt.xlabel(r"$\xi$ / deg")
if args.write:
save_fig('{}/reco_xi_{}'.format(args.plots_dir, args.mode))
plt.pause(.1)
plt.figure()
plt.hist(reco_table.cols.ErrEstDir[:], bins=np.linspace(0, 20, 50))
plt.title(channel)
plt.xlabel("beta")
plt.pause(.1)
plt.figure()
plt.hist(np.log10(reco_table.cols.xi[:] / reco_table.cols.ErrEstDir[:]),
bins=50)
plt.title(channel)
plt.xlabel("log_10(xi / beta)")
plt.pause(.1)
# convert the xi-list into a dict with the number of used telescopes as keys
xi_vs_tel = {}
for xi, ntel in zip(reco_table.cols.xi, reco_table.cols.NTels_clean):
if ntel not in xi_vs_tel:
xi_vs_tel[ntel] = [xi]
else:
xi_vs_tel[ntel].append(xi)
print(args.mode)
for ntel, xis in sorted(xi_vs_tel.items()):
print("NTel: {} -- median xi: {}".format(ntel, np.median(xis)))
# print("histogram:", np.histogram(xis, bins=xi_edges))
# create a list of energy bin-edges and -centres for violin plots
Energy_edges = np.linspace(2, 8, 13)
Energy_centres = (Energy_edges[1:] + Energy_edges[:-1]) / 2.
# convert the xi-list in to an energy-binned dict with the bin centre as keys
xi_vs_energy = {}
for en, xi in zip(reco_table.cols.EnMC, reco_table.cols.xi):
# get the bin number this event belongs into
sbin = np.digitize(np.log10(en), Energy_edges) - 1
# the central value of the bin is the key for the dictionary
if Energy_centres[sbin] not in xi_vs_energy:
xi_vs_energy[Energy_centres[sbin]] = [xi]
else:
xi_vs_energy[Energy_centres[sbin]] += [xi]
# plotting the angular error as violin plots with binning in
# number of telescopes and shower energy
figure = plt.figure()
plt.subplot(211)
plt.violinplot([np.log10(a) for a in xi_vs_tel.values()],
[a for a in xi_vs_tel.keys()],
points=60,
widths=.75,
showextrema=False,
showmedians=True)
plt.xlabel("Number of Telescopes")
plt.ylabel(r"log($\xi$ / deg)")
plt.ylim(-3, 2)
plt.grid()
plt.subplot(212)
plt.violinplot([np.log10(a) for a in xi_vs_energy.values()],
[a for a in xi_vs_energy.keys()],
points=60,
widths=(Energy_edges[1] - Energy_edges[0]) / 1.5,
showextrema=False,
showmedians=True)
plt.xlabel(r"log(Energy / GeV)")
plt.ylabel(r"log($\xi$ / deg)")
plt.ylim(-3, 2)
plt.grid()
plt.tight_layout()
if args.write:
save_fig('{}/reco_xi_vs_E_NTel_{}'.format(args.plots_dir, args.mode))
plt.pause(.1)
# convert the diffs-list into a dict with the number of used telescopes as keys
diff_vs_tel = {}
for diff, ntel in zip(reco_table.cols.DeltaR, reco_table.cols.NTels_clean):
if ntel not in diff_vs_tel:
diff_vs_tel[ntel] = [diff]
else:
diff_vs_tel[ntel].append(diff)
# convert the diffs-list in to an energy-binned dict with the bin centre as keys
diff_vs_energy = {}
for en, diff in zip(reco_table.cols.EnMC, reco_table.cols.DeltaR):
# get the bin number this event belongs into
sbin = np.digitize(np.log10(en), Energy_edges) - 1
# the central value of the bin is the key for the dictionary
if Energy_centres[sbin] not in diff_vs_energy:
diff_vs_energy[Energy_centres[sbin]] = [diff]
else:
diff_vs_energy[Energy_centres[sbin]] += [diff]
# plotting the core position error as violin plots with binning in
# number of telescopes an shower energy
plt.figure()
plt.subplot(211)
plt.violinplot([np.log10(a) for a in diff_vs_tel.values()],
[a for a in diff_vs_tel.keys()],
points=60,
widths=.75,
showextrema=False,
showmedians=True)
plt.xlabel("Number of Telescopes")
plt.ylabel(r"log($\Delta R$ / m)")
plt.grid()
plt.subplot(212)
plt.violinplot([np.log10(a) for a in diff_vs_energy.values()],
[a for a in diff_vs_energy.keys()],
points=60,
widths=(Energy_edges[1] - Energy_edges[0]) / 1.5,
showextrema=False,
showmedians=True)
plt.xlabel(r"log(Energy / GeV)")
plt.ylabel(r"log($\Delta R$ / m)")
plt.grid()
plt.tight_layout()
if args.write:
save_fig('{}/reco_dist_vs_E_NTel_{}'.format(args.plots_dir, args.mode))
plt.show()
# pointing direction of the telescopes
point_azimuth = {}
point_altitude = {}
reco = HillasReconstructor()
calib = CameraCalibrator(r1_product="HESSIOR1Calibrator")
off_angles = []
for event in source:
# The direction the incident particle.
# Converting Monte Carlo Shower parameter theta and phi to
# corresponding to 3 components (x,y,z) of a vector
shower_azimuth = event.mc.az # same as in Monte Carlo file i.e. phi
shower_altitude = np.pi * u.rad / 2 - event.mc.alt # altitude = 90 - theta
shower_direction = linalg.set_phi_theta(shower_azimuth, shower_altitude)
# calibrating the event
calib.calibrate(event)
hillas_params = {}
subarray = event.inst.subarray
for tel_id in event.dl0.tels_with_data:
# telescope pointing direction
point_azimuth[tel_id] = event.mc.tel[tel_id].azimuth_raw * u.rad
point_altitude[tel_id] = (np.pi / 2 - event.mc.tel[tel_id].altitude_raw) * u.rad
# print(point_azimuth,point_altitude)
# Camera Geometry required for hillas parametrization
pix_x = subarray.tel[tel_id].camera.pix_x
pix_y = subarray.tel[tel_id].camera.pix_y
allowed_tels = prod3b_tel_ids("CHEC")
for filename in sorted(filenamelist)[:args.last]:
print("filename = {}".format(filename))
source = hessio_event_source(filename,
allowed_tels=allowed_tels,
max_events=args.max_events)
for event in source:
print()
print('Available telscopes: {}'.format(event.dl0.tels_with_data))
# getting the MC shower info
shower = event.mc
shower_org = linalg.set_phi_theta(shower.az,
90. * u.deg - shower.alt)
shower_org = linalg.set_phi_theta(90 * u.deg - shower.az,
90. * u.deg - shower.alt)
org_alt = u.Quantity(shower.alt).to(u.deg)
org_az = u.Quantity(shower.az).to(u.deg)
if org_az > 180 * u.deg:
org_az -= 360 * u.deg
org_the = alt_to_theta(org_alt)
org_phi = az_to_phi(org_az)
shower_org = linalg.set_phi_theta(org_phi, org_the)
# calibrate the event
calib.calibrate(event)
def main():
# your favourite units here
energy_unit = u.TeV
angle_unit = u.deg
dist_unit = u.m
agree_threshold = .5
min_tel = 3
parser = make_argparser()
parser.add_argument('--classifier', type=str,
default='data/classifier_pickle/classifier'
'_{mode}_{cam_id}_{classifier}.pkl')
parser.add_argument('--regressor', type=str,
default='data/classifier_pickle/regressor'
'_{mode}_{cam_id}_{regressor}.pkl')
parser.add_argument('-o', '--outfile', type=str, default="",
help="location to write the classified events to.")
parser.add_argument('--wave_dir', type=str, default=None,
help="directory where to find mr_filter. "
"if not set look in $PATH")
parser.add_argument('--wave_temp_dir', type=str, default='/tmp/', help="directory "
"where mr_filter to store the temporary fits files")
group = parser.add_mutually_exclusive_group()
group.add_argument('--proton', action='store_true',
help="do protons instead of gammas")
group.add_argument('--electron', action='store_true',
help="do electrons instead of gammas")
args = parser.parse_args()
if args.infile_list:
filenamelist = []
for f in args.infile_list:
filenamelist += glob("{}/{}".format(args.indir, f))
filenamelist.sort()
elif args.proton:
filenamelist = sorted(glob("{}/proton/*gz".format(args.indir)))
elif args.electron:
filenamelist = glob("{}/electron/*gz".format(args.indir))
channel = "electron"
else:
filenamelist = sorted(glob("{}/gamma/*gz".format(args.indir)))
if not filenamelist:
print("no files found; check indir: {}".format(args.indir))
exit(-1)
# keeping track of events and where they were rejected
Eventcutflow = CutFlow("EventCutFlow")
Imagecutflow = CutFlow("ImageCutFlow")
# takes care of image cleaning
cleaner = ImageCleaner(mode=args.mode, cutflow=Imagecutflow,
wavelet_options=args.raw,
skip_edge_events=False, island_cleaning=True)
# the class that does the shower reconstruction
shower_reco = HillasReconstructor()
preper = EventPreparer(
cleaner=cleaner, hillas_parameters=hillas_parameters,
shower_reco=shower_reco,
event_cutflow=Eventcutflow, image_cutflow=Imagecutflow,
# event/image cuts:
allowed_cam_ids=[],
min_ntel=2, min_charge=args.min_charge, min_pixel=3)
# wrapper for the scikit-learn classifier
classifier = EventClassifier.load(
args.classifier.format(**{
"mode": args.mode,
"wave_args": "mixed",
"classifier": 'RandomForestClassifier',
"cam_id": "{cam_id}"}),
cam_id_list=args.cam_ids)
# wrapper for the scikit-learn regressor
regressor = EnergyRegressor.load(
args.regressor.format(**{
"mode": args.mode,
"wave_args": "mixed",
"regressor": "RandomForestRegressor",
"cam_id": "{cam_id}"}),
cam_id_list=args.cam_ids)
ClassifierFeatures = namedtuple(
"ClassifierFeatures", (
"impact_dist",
"sum_signal_evt",
"max_signal_cam",
"sum_signal_cam",
"N_LST",
"N_MST",
"N_SST",
"width",
"length",
"skewness",
"kurtosis",
"h_max",
"err_est_pos",
"err_est_dir"))
EnergyFeatures = namedtuple(
"EnergyFeatures", (
"impact_dist",
"sum_signal_evt",
"max_signal_cam",
"sum_signal_cam",
"N_LST",
"N_MST",
"N_SST",
"width",
"length",
"skewness",
"kurtosis",
"h_max",
"err_est_pos",
"err_est_dir"))
# catch ctr-c signal to exit current loop and still display results
signal_handler = SignalHandler()
signal.signal(signal.SIGINT, signal_handler)
# this class defines the reconstruction parameters to keep track of
class RecoEvent(tb.IsDescription):
Run_ID = tb.Int16Col(dflt=-1, pos=0)
Event_ID = tb.Int16Col(dflt=-1, pos=1)
NTels_trig = tb.Int16Col(dflt=0, pos=0)
NTels_reco = tb.Int16Col(dflt=0, pos=1)
NTels_reco_lst = tb.Int16Col(dflt=0, pos=2)
NTels_reco_mst = tb.Int16Col(dflt=0, pos=3)
NTels_reco_sst = tb.Int16Col(dflt=0, pos=4)
MC_Energy = tb.Float32Col(dflt=np.nan, pos=5)
reco_Energy = tb.Float32Col(dflt=np.nan, pos=6)
reco_phi = tb.Float32Col(dflt=np.nan, pos=7)
reco_theta = tb.Float32Col(dflt=np.nan, pos=8)
off_angle = tb.Float32Col(dflt=np.nan, pos=9)
xi = tb.Float32Col(dflt=np.nan, pos=10)
DeltaR = tb.Float32Col(dflt=np.nan, pos=11)
ErrEstPos = tb.Float32Col(dflt=np.nan, pos=12)
ErrEstDir = tb.Float32Col(dflt=np.nan, pos=13)
gammaness = tb.Float32Col(dflt=np.nan, pos=14)
channel = "gamma" if "gamma" in " ".join(filenamelist) else "proton"
reco_outfile = tb.open_file(
mode="w",
# if no outfile name is given (i.e. don't to write the event list to disk),
# need specify two "driver" arguments
**({"filename": args.outfile} if args.outfile else
{"filename": "no_outfile.h5",
"driver": "H5FD_CORE", "driver_core_backing_store": False}))
reco_table = reco_outfile.create_table("/", "reco_events", RecoEvent)
reco_event = reco_table.row
allowed_tels = None # all telescopes
allowed_tels = prod3b_tel_ids("L+N+D")
for i, filename in enumerate(filenamelist[:args.last]):
# print(f"file: {i} filename = {filename}")
source = hessio_event_source(filename,
allowed_tels=allowed_tels,
max_events=args.max_events)
# loop that cleans and parametrises the images and performs the reconstruction
for (event, hillas_dict, n_tels,
tot_signal, max_signals, pos_fit, dir_fit, h_max,
err_est_pos, err_est_dir) in preper.prepare_event(source, True):
# now prepare the features for the classifier
cls_features_evt = {}
reg_features_evt = {}
if hillas_dict is not None:
for tel_id in hillas_dict.keys():
Imagecutflow.count("pre-features")
tel_pos = np.array(event.inst.tel_pos[tel_id][:2]) * u.m
moments = hillas_dict[tel_id]
impact_dist = linalg.length(tel_pos - pos_fit)
cls_features_tel = ClassifierFeatures(
impact_dist=impact_dist / u.m,
sum_signal_evt=tot_signal,
max_signal_cam=max_signals[tel_id],
sum_signal_cam=moments.size,
N_LST=n_tels["LST"],
N_MST=n_tels["MST"],
N_SST=n_tels["SST"],
width=moments.width / u.m,
length=moments.length / u.m,
skewness=moments.skewness,
kurtosis=moments.kurtosis,
h_max=h_max / u.m,
err_est_pos=err_est_pos / u.m,
err_est_dir=err_est_dir / u.deg
)
reg_features_tel = EnergyFeatures(
impact_dist=impact_dist / u.m,
sum_signal_evt=tot_signal,
max_signal_cam=max_signals[tel_id],
sum_signal_cam=moments.size,
N_LST=n_tels["LST"],
N_MST=n_tels["MST"],
N_SST=n_tels["SST"],
width=moments.width / u.m,
length=moments.length / u.m,
skewness=moments.skewness,
kurtosis=moments.kurtosis,
h_max=h_max / u.m,
err_est_pos=err_est_pos / u.m,
err_est_dir=err_est_dir / u.deg
)
if np.isnan(cls_features_tel).any() or np.isnan(reg_features_tel).any():
continue
Imagecutflow.count("features nan")
cam_id = event.inst.subarray.tel[tel_id].camera.cam_id
try:
reg_features_evt[cam_id] += [reg_features_tel]
cls_features_evt[cam_id] += [cls_features_tel]
except KeyError:
reg_features_evt[cam_id] = [reg_features_tel]
cls_features_evt[cam_id] = [cls_features_tel]
# save basic event infos
reco_event["MC_Energy"] = event.mc.energy.to(energy_unit).value
reco_event["Event_ID"] = event.r1.event_id
reco_event["Run_ID"] = event.r1.run_id
if cls_features_evt and reg_features_evt:
predict_energ = regressor.predict_by_event([reg_features_evt])["mean"][0]
predict_proba = classifier.predict_proba_by_event([cls_features_evt])
gammaness = predict_proba[0, 0]
# the MC direction of origin of the simulated particle
shower = event.mc
shower_core = np.array([shower.core_x / u.m, shower.core_y / u.m]) * u.m
shower_org = linalg.set_phi_theta(shower.az + 90 * u.deg,
90. * u.deg - shower.alt)
# and how the reconstructed direction compares to that
xi = linalg.angle(dir_fit, shower_org)
phi, theta = linalg.get_phi_theta(dir_fit)
phi = (phi if phi > 0 else phi + 360 * u.deg)
DeltaR = linalg.length(pos_fit[:2] - shower_core)
# TODO: replace with actual array pointing direction
array_pointing = linalg.set_phi_theta(0 * u.deg, 20. * u.deg)
# angular offset between the reconstructed direction and the array
# pointing
off_angle = linalg.angle(dir_fit, array_pointing)
reco_event["NTels_trig"] = len(event.dl0.tels_with_data)
reco_event["NTels_reco"] = len(hillas_dict)
reco_event["NTels_reco_lst"] = n_tels["LST"]
reco_event["NTels_reco_mst"] = n_tels["MST"]
reco_event["NTels_reco_sst"] = n_tels["SST"]
reco_event["reco_Energy"] = predict_energ.to(energy_unit).value
reco_event["reco_phi"] = phi / angle_unit
reco_event["reco_theta"] = theta / angle_unit
reco_event["off_angle"] = off_angle / angle_unit
reco_event["xi"] = xi / angle_unit
reco_event["DeltaR"] = DeltaR / dist_unit
reco_event["ErrEstPos"] = err_est_pos / dist_unit
reco_event["ErrEstDir"] = err_est_dir / angle_unit
reco_event["gammaness"] = gammaness
reco_event.append()
reco_table.flush()
if signal_handler.stop:
break
if signal_handler.stop:
break
try:
print()
Eventcutflow()
print()
Imagecutflow()
# do some simple event selection
# and print the corresponding selection efficiency
N_selected = len([x for x in reco_table.where(
"""(NTels_reco > min_tel) & (gammaness > agree_threshold)""")])
N_total = len(reco_table)
print("\nfraction selected events:")
print("{} / {} = {} %".format(N_selected, N_total, N_selected / N_total * 100))
except ZeroDivisionError:
pass
print("\nlength filenamelist:", len(filenamelist[:args.last]))
# do some plotting if so desired
if args.plot:
gammaness = [x['gammaness'] for x in reco_table]
NTels_rec = [x['NTels_reco'] for x in reco_table]
NTel_bins = np.arange(np.min(NTels_rec), np.max(NTels_rec) + 2) - .5
NTels_rec_lst = [x['NTels_reco_lst'] for x in reco_table]
NTels_rec_mst = [x['NTels_reco_mst'] for x in reco_table]
NTels_rec_sst = [x['NTels_reco_sst'] for x in reco_table]
reco_energy = np.array([x['reco_Energy'] for x in reco_table])
mc_energy = np.array([x['MC_Energy'] for x in reco_table])
fig = plt.figure(figsize=(15, 5))
plt.suptitle(" ** ".join([args.mode, "protons" if args.proton else "gamma"]))
plt.subplots_adjust(left=0.05, right=0.97, hspace=0.39, wspace=0.2)
ax = plt.subplot(131)
histo = np.histogram2d(NTels_rec, gammaness,
bins=(NTel_bins, np.linspace(0, 1, 11)))[0].T
histo_normed = histo / histo.max(axis=0)
im = ax.imshow(histo_normed, interpolation='none', origin='lower',
aspect='auto',
# extent=(*NTel_bins[[0, -1]], 0, 1),
cmap=plt.cm.inferno)
ax.set_xlabel("NTels")
ax.set_ylabel("drifted gammaness")
plt.title("Total Number of Telescopes")
# next subplot
ax = plt.subplot(132)
histo = np.histogram2d(NTels_rec_sst, gammaness,
bins=(NTel_bins, np.linspace(0, 1, 11)))[0].T
histo_normed = histo / histo.max(axis=0)
im = ax.imshow(histo_normed, interpolation='none', origin='lower',
aspect='auto',
# extent=(*NTel_bins[[0, -1]], 0, 1),
cmap=plt.cm.inferno)
ax.set_xlabel("NTels")
plt.setp(ax.get_yticklabels(), visible=False)
plt.title("Number of SSTs")
# next subplot
ax = plt.subplot(133)
histo = np.histogram2d(NTels_rec_mst, gammaness,
bins=(NTel_bins, np.linspace(0, 1, 11)))[0].T
histo_normed = histo / histo.max(axis=0)
im = ax.imshow(histo_normed, interpolation='none', origin='lower',
aspect='auto',
# extent=(*NTel_bins[[0, -1]], 0, 1),
cmap=plt.cm.inferno)
cb = fig.colorbar(im, ax=ax)
ax.set_xlabel("NTels")
plt.setp(ax.get_yticklabels(), visible=False)
plt.title("Number of MSTs")
plt.subplots_adjust(wspace=0.05)
# plot the energy migration matrix
plt.figure()
plt.hist2d(np.log10(reco_energy), np.log10(mc_energy), bins=20,
cmap=plt.cm.inferno)
plt.xlabel("E_MC / TeV")
plt.ylabel("E_rec / TeV")
plt.colorbar()
plt.show()