def recorrect_s2xy(
data,
old_map_file='s2_xy_XENON1T_17Feb2017.json',
new_map_file=pax_config['WaveformSimulator']['s2_light_yield_map']):
"""Recompute the (x,y) correction for a different map
:param data: dataframe (Basics and Extended minitrees required)
:param old_map_file: Map filename that was used to process the dataframe. Defaults to the map used for 6.4.2
:param new_map_file: Map filename that you want to use for the correction. Defaults to the pax config default.
:return: dataframe with altered value in cS2 (and few added columns for uncorrected position)
TODO: This could be rewritten to use the extended minitrees, so the old map no longer needs to be specified.
"""
data = data.copy()
add_uncorrected_position(data)
old_map = InterpolatingMap(data_file_name(old_map_file))
new_map = InterpolatingMap(data_file_name(new_map_file))
# Correction is a *division* factor (map contains light yield), so to un-correct we first multiply
recorrection = np.zeros(len(data))
x = data._u_x.values
y = data._u_y.values
for i in tqdm(range(len(data))):
recorrection[i] = old_map.get_value(x[i], y[i]) / new_map.get_value(
x[i], y[i])
data['cs2'] *= recorrection
return data
def load_nn(self):
"""For loading NN files"""
from keras.models import model_from_json
# If we already loaded it up then skip
if ((self.tfnn_weights == self.corrections_handler.get_misc_correction(
"tfnn_weights", self.run_number)) and
(self.tfnn_model == self.corrections_handler.get_misc_correction(
"tfnn_model", self.run_number))):
return
self.tfnn_weights = self.corrections_handler.get_misc_correction(
"tfnn_weights", self.run_number)
self.tfnn_model = self.corrections_handler.get_misc_correction(
"tfnn_model", self.run_number)
json_file_nn = open(utils.data_file_name(self.tfnn_model), 'r')
loaded_model_json = json_file_nn.read()
self.loaded_nn = model_from_json(loaded_model_json)
json_file_nn.close()
# Get bad PMT List in JSON file:
json_file_nn = open(utils.data_file_name(self.tfnn_model), 'r')
loaded_model_json_dict = json.load(json_file_nn)
self.list_bad_pmts = loaded_model_json_dict['badPMTList']
json_file_nn.close()
weights_file = utils.data_file_name(self.tfnn_weights)
self.loaded_nn.load_weights(weights_file)
def __init__(self):
hax.minitrees.TreeMaker.__init__(self)
self.extra_metadata = hax.config['corrections_definitions']
self.corrections_handler = CorrectionsHandler()
# We need to pull some stuff from the pax config
self.pax_config = load_configuration("XENON1T")
self.tpc_channels = self.pax_config['DEFAULT']['channels_in_detector']['tpc']
self.confused_s1_channels = []
self.s1_statistic = (
self.pax_config['BuildInteractions.BasicInteractionProperties']['s1_pattern_statistic']
)
qes = np.array(self.pax_config['DEFAULT']['quantum_efficiencies'])
self.s1_pattern_fitter = PatternFitter(
filename=utils.data_file_name(self.pax_config['WaveformSimulator']['s1_patterns_file']),
zoom_factor=self.pax_config['WaveformSimulator'].get('s1_patterns_zoom_factor', 1),
adjust_to_qe=qes[self.tpc_channels],
default_errors=(self.pax_config['DEFAULT']['relative_qe_error'] +
self.pax_config['DEFAULT']['relative_gain_error'])
)
self.top_channels = self.pax_config['DEFAULT']['channels_top']
self.ntop_pmts = len(self.top_channels)
# Declare nn stuff
self.tfnn_weights = None
self.tfnn_model = None
self.loaded_nn = None
# Run doc
self.loaded_run_doc = None
self.run_doc = None
def startup(self):
""" Initialize the neural net.
"""
if self.config['pmt_0_is_fake']:
self.input_channels = self.pmts[1:]
else:
self.input_channels = self.pmts
self.nn_output_unit = self.config['nn_output_unit']
# Possibly scale the input of the activation function by a supplied value (float)
activation_scale = self.config['activation_function_scale']
# Apply the activation function to the output layer (bool)
output_layer_function = self.config['output_layer_function']
# Load the file defining the structure (number of nodes per layer)
# as well as the weights and biases of the neural network
data = np.load(utils.data_file_name(self.config['neural_net_file']))
self.nn = NeuralNet(structure=data['structure'],
weights=data['weights'],
biases=data['biases'],
activation_scale=activation_scale,
output_layer_function=output_layer_function)
data.close()
def recorrect_rz(data, new_map_file=None):
"""Recompute the (r,z)(r,z) field distortion correction
Be sure to redo the S1(x,y,z) correction after this as well, whether or not the S1(x,y,z) map changed!
:param data: input dataframe
:param new_map_file: file with (r,z)(r,z) correction map to use. Defaults to map currently in pax config.
:return: dataframe with altered values in x, y, z (and few added columns for uncorrected position)
"""
if new_map_file is None:
# Specified here, since older pax versions do not have this map defined
return pax_config['WaveformSimulator']['rz_position_distortion_map']
data = data.copy()
add_uncorrected_position(data)
# Compute correction for new map
new_map = InterpolatingMap(data_file_name(new_map_file))
r_corr = np.zeros(len(data))
z_corr = np.zeros(len(data))
_u_r = data._u_r.values
_u_z = data._u_z.values
for i in tqdm(range(len(data)), desc="Redoing (r,z) correction"):
r_corr[i] = new_map.get_value(_u_r[i], _u_z[i], map_name='to_true_r')
z_corr[i] = new_map.get_value(_u_r[i], _u_z[i], map_name='to_true_z')
data['r'] = data._u_r + r_corr
data['x'] = data.r * np.cos(data.theta)
data['y'] = data.r * np.sin(data.theta)
data['z'] = data._u_z + z_corr
return data
def startup(self):
""" Initialize the neural net.
"""
if self.config['pmt_0_is_fake']:
self.input_channels = self.pmts[1:]
else:
self.input_channels = self.pmts
self.nn_output_unit = self.config['nn_output_unit']
# Possibly scale the input of the activation function by a supplied value (float)
activation_scale = self.config['activation_function_scale']
# Apply the activation function to the output layer (bool)
output_layer_function = self.config['output_layer_function']
# Load the file defining the structure (number of nodes per layer)
# as well as the weights and biases of the neural network
data = np.load(utils.data_file_name(self.config['neural_net_file']))
self.nn = NeuralNet(structure=data['structure'],
weights=data['weights'],
biases=data['biases'],
activation_scale=activation_scale,
output_layer_function=output_layer_function)
data.close()
def startup(self):
self.raw_data_files = []
self.current_file_number = None
self.current_filename = None
self.current_first_event = None
self.current_last_event = None
input_name = utils.data_file_name(self.config['input_name'])
if not os.path.exists(input_name):
raise ValueError("Can't read from %s: it does not exist!" %
input_name)
if not os.path.isdir(input_name):
if not input_name.endswith('.' + self.file_extension):
self.log.error("input_name %s does not end "
"with the expected file extension %s" %
(input_name, self.file_extension))
return
self.log.debug("InputFromFolder: Single file mode")
self.init_file(input_name)
else:
self.log.debug("InputFromFolder: Directory mode")
file_names = glob.glob(
os.path.join(input_name, "*." + self.file_extension))
# Remove the pax_info.json file from the file list-- the JSON I/O will thank us
file_names = [
fn for fn in file_names if not fn.endswith('pax_info.json')
]
file_names.sort()
self.log.debug("InputFromFolder: Found these files: %s",
str(file_names))
if len(file_names) == 0:
raise ValueError(
"InputFromFolder: No %s files found in input directory %s!"
% (self.file_extension, input_name))
for fn in file_names:
if 'trigger_monitor_data.' in fn:
continue
if 'temp.' in fn:
self.log.warning(
"Temporary raw data file found in directory: this data is still being built "
"or has crashed while building!")
continue
self.init_file(fn)
# Sort the files by first event number, so events are read in order
# Files are read in lexically, but in some cases that may not reflect the event order (see issue #345)
self.raw_data_files = sorted(self.raw_data_files,
key=itemgetter('first_event'))
# Select the first file
self.select_file(0)
# Set the number of total events
self.number_of_events = sum(
[fr['n_events'] for fr in self.raw_data_files])
def startup(self):
if not have_root:
raise RuntimeError("Can't read MC ROOT files if you do not have root!")
self.config.setdefault('add_to_z', 0)
self.log.warning('This plugin is completely untested and will probably crash!')
filename = self.config['input_name']
self.f = ROOT.TFile(utils.data_file_name(filename))
self.t = self.f.Get("events/events") # new MC structure, 160622
WaveformSimulator.startup(self)
self.number_of_events = self.t.GetEntries() * self.config['event_repetitions']
def startup(self):
# Call original startup function
PosRecTopPatternFit.startup(self)
# Get the Fax config
c = self.processor.simulator.config
qes = np.array(c['quantum_efficiencies'])
# Change the pattern fitter instance so it uses TPFF
self.pf = PatternFitter(
filename=utils.data_file_name(c['s2_fitted_patterns_file']),
zoom_factor=c.get('s2_fitted_patterns_zoom_factor', 1),
adjust_to_qe=qes[c['channels_top']],
default_errors=c['relative_qe_error'] + c['relative_gain_error'])
def startup(self):
if not have_root:
raise RuntimeError(
"Can't read MC ROOT files if you do not have root!")
self.config.setdefault('add_to_z', 0)
self.log.warning(
'This plugin is completely untested and will probably crash!')
filename = self.config['input_name']
self.f = ROOT.TFile(utils.data_file_name(filename))
self.t = self.f.Get("events/events") # new MC structure, 160622
WaveformSimulator.startup(self)
self.number_of_events = self.t.GetEntries(
) * self.config['event_repetitions']
def __init__(self, zoom_multiplier=1):
# Get some settings from the XENON1T detector configuration
config = load_configuration('XENON1T')
# The per-PMT S2 LCE maps (and zoom factor which is a technical detail)
lce_maps = config['WaveformSimulator']['s2_patterns_file']
lce_map_zoom = config['WaveformSimulator']['s2_patterns_zoom_factor']
# Simulate the right PMT response
qes = np.array(config['DEFAULT']['quantum_efficiencies'])
top_pmts = config['DEFAULT']['channels_top']
errors = config['DEFAULT']['relative_qe_error'] + config['DEFAULT'][
'relative_gain_error']
# Set up the PatternFitter which sample the LCE maps
self.pf = PatternFitter(filename=utils.data_file_name(lce_maps),
zoom_factor=lce_map_zoom * zoom_multiplier,
adjust_to_qe=qes[top_pmts],
default_errors=errors)
def startup(self):
"""
The startup routine of the WaveformSimulatorFromCSV plugin
"""
# Open the instructions file
filename = self.config['input_name']
self.dataset_name = os.path.basename(filename)
self.instructions_file = open(utils.data_file_name(filename), 'r')
#
# Slurp the entire instructions file, so we know the number of events
self.instruction_reader = csv.DictReader(self.instructions_file)
self.instructions = []
#
# Loop over lines, make instructions
instruction_number = 0
instruction = []
for p in self.instruction_reader:
p['g4_id'] = -1 # create fake g4_id=-1 for csv input
if p['depth'] == 'random':
p['z'] = 'random'
else:
p['z'] = -1 * float(p['depth'])
del p['depth']
if int(p['instruction']) == instruction_number:
# Deposition is part of the previous instruction
instruction.append(p)
else:
# New deposition reached!
if instruction:
self.instructions.append(instruction)
instruction_number = int(p['instruction'])
instruction = [p]
# For the final instruction
self.instructions.append(instruction)
self.number_of_events = len(
self.instructions) * self.config['event_repetitions']
WaveformSimulator.startup(self)
def startup(self):
"""
The startup routine of the WaveformSimulatorFromCSV plugin
"""
# Open the instructions file
filename = self.config['input_name']
self.dataset_name = os.path.basename(filename)
self.instructions_file = open(utils.data_file_name(filename), 'r')
#
# Slurp the entire instructions file, so we know the number of events
self.instruction_reader = csv.DictReader(self.instructions_file)
self.instructions = []
#
# Loop over lines, make instructions
instruction_number = 0
instruction = []
for p in self.instruction_reader:
p['g4_id'] = -1 # create fake g4_id=-1 for csv input
if p['depth'] == 'random':
p['z'] = 'random'
else:
p['z'] = -1 * float(p['depth'])
del p['depth']
if int(p['instruction']) == instruction_number:
# Deposition is part of the previous instruction
instruction.append(p)
else:
# New deposition reached!
if instruction:
self.instructions.append(instruction)
instruction_number = int(p['instruction'])
instruction = [p]
# For the final instruction
self.instructions.append(instruction)
self.number_of_events = len(self.instructions) * self.config['event_repetitions']
WaveformSimulator.startup(self)
def startup(self):
""" Initialize the neural net.
"""
if self.config['pmt_0_is_fake']:
self.input_channels = self.pmts[1:]
else:
self.input_channels = self.pmts
activation_scale = 0.5
output_layer_function = True
self.nn_output_unit = self.config['nn_output_unit']
# Load the file defining the structure (number of nodes per layer)
# as well as the weights and biases of the neural network
data = np.load(utils.data_file_name(self.config['neural_net_file']))
self.nn = NeuralNet(structure=data['structure'],
weights=data['weights'],
biases=data['biases'],
activation_scale=activation_scale,
output_layer_function=output_layer_function)
data.close()
def recorrect_s1xyz(
data,
new_map_file=pax_config['WaveformSimulator']['s1_light_yield_map']):
"""Recompute the S1(x,y,z) light yield correction.
If you want to redo (r,z)(r,z), do it before doing this!
:param data: Dataframe. Only Basics minitree required.
:param new_map_name: Filename of map you want to use for the correction.
:return: Dataframe with changed values in cs1 column
"""
new_map = InterpolatingMap(data_file_name(new_map_file))
# Correction is a *division* factor (map contains light yield)
x = data.x.values
y = data.y.values
z = data.z.values
correction = np.zeros(len(data))
for i in tqdm(range(len(data)), desc='Redoing S1(x,y,z) correction'):
correction[i] = 1 / new_map.get_value(x[i], y[i], z[i])
data['cs1'] = data['s1'] * correction
return data
def __init__(self,
filename,
zoom_factor=1,
adjust_to_qe=None,
default_errors=None):
"""Initialize a pattern map file from filename.
Format of the file is very similar to InterpolatingMap; a (gzip compressed) json containing:
'coordinate_system' : [['x', (x_min, x_max, n_x)], ['y',...
'map' : [[[valuex1y1pmt1, valuex1y1pmt2, ...], ...], ...]
'name': 'Nice file with maps',
'description': 'Say what the maps are, who you are, your favorite food, etc',
'timestamp': unix epoch seconds timestamp
where x_min is the lowest x coordinate of a point, x_max the highest, n_x the number of points
zoom_factor is factor by which the spatial dimensions of the map will be upsampled.
adjust_to_qe: array of same length as the number of pmts in the map;
we'll adjust the patterns to account for these QEs, upweighing PMTs with higher QEs
Obviously this should be None if map already includes QE effects (e.g. if it is data-derived)!
default_errors: array of the same length as the number of pmts in the map;
This is the default factor which will be applied to obtain the squared systematic errors in the goodness
of fit statistic, as follows:
squared_systematic_errors = (areas_observed * default_errors)**2
"""
self.log = logging.getLogger('PatternFitter')
with gzip.open(utils.data_file_name(filename)) as infile:
json_data = json.loads(infile.read().decode())
self.data = np.array(json_data['map'])
self.log.debug('Loaded pattern file named: %s' % json_data['name'])
self.log.debug('Description:\n ' +
re.sub(r'\n', r'\n ', json_data['description']))
self.log.debug('Data shape: %s' % str(self.data.shape))
self.log.debug('Will zoom in by factor %s' % zoom_factor)
self.dimensions = len(
json_data['coordinate_system']
) # Spatial dimensions (other one is sampling points)
# Zoom the spatial map using linear interpolation, if desired
if zoom_factor != 1:
self.data = image_zoom(self.data,
zoom=[zoom_factor] * self.dimensions + [1],
order=1)
# Adjust the expected patterns to the PMT's quantum efficiencies, if desired
# No need to re-normalize: will be done in each gof computation anyway
if adjust_to_qe is not None:
self.data *= adjust_to_qe[[np.newaxis] * self.dimensions]
# Store index starts and distances for quick access, assuming uniform grid spacing
self.coordinate_data = []
for dim_i, (name,
(start, stop,
n_points)) in enumerate(json_data['coordinate_system']):
n_points *= zoom_factor
if not n_points == self.data.shape[dim_i]:
raise ValueError(
"Map interpretation error: %d points expected along %s, but map is %d points long"
% (n_points, name, self.data.shape[dim_i]))
self.coordinate_data.append(
CoordinateData(minimum=start,
maximum=stop,
n_points=n_points,
point_spacing=(stop - start) / (n_points - 1)))
self.log.debug('Coordinate ranges: %s' % ', '.join([
'%s-%s (%d points)' % (cd.minimum, cd.maximum, cd.n_points)
for cd in self.coordinate_data
]))
# TODO: Technically we should zero the points outside the tpc bounds again:
# some LCE may have leaked into this region due to upsampling... but doesn't matter:
# if it causes a bias, it will push some events who are already far outside the fiducial volume
# even further out.
self.n_points = self.data.shape[-1]
self.default_pmt_selection = np.ones(self.n_points, dtype=np.bool)
if default_errors is None:
default_errors = 0
self.default_errors = default_errors
def startup(self):
aftmap_filename = utils.data_file_name('XENON1T_s1_aft_xyz_20170808.json')
self.aft_map = InterpolatingMap(aftmap_filename)
def startup(self):
aftmap_filename = utils.data_file_name('s1_aft_xyz_XENON1T_06Mar2017.json')
self.aft_map = InterpolatingMap(aftmap_filename)
self.low_pe_threshold = 10 # below this in PE, transition to hits
def __init__(self, config_to_init):
c = self.config = config_to_init
# Should we repeat events?
if 'event_repetitions' not in c:
c['event_repetitions'] = 1
# Primary excimer fraction from Nest Version 098
# See G4S1Light.cc line 298
density = c['liquid_density'] / (units.g / units.cm**3)
excfrac = 0.4 - 0.11131 * density - 0.0026651 * density**2 # primary / secondary excimers
excfrac = 1 / (1 + excfrac) # primary / all excimers
# primary / all excimers that produce a photon:
excfrac /= 1 - (1 - excfrac) * (1 - c['s1_ER_recombination_fraction'])
c['s1_ER_primary_excimer_fraction'] = excfrac
log.debug('Inferred s1_ER_primary_excimer_fraction %s' % excfrac)
# Recombination time from NEST 2014
# 3.5 seems fishy, they fit an exponential to data, but in the code they use a non-exponential distribution...
efield = (c['drift_field'] / (units.V / units.cm))
c['s1_ER_recombination_time'] = 3.5 / 0.18 * (
1 / 20 + 0.41) * math.exp(-0.009 * efield)
log.debug('Inferred s1_ER_recombination_time %s ns' %
c['s1_ER_recombination_time'])
# Which channels stand to receive any photons?
channels_for_photons = c['channels_in_detector']['tpc']
if c['pmt_0_is_fake']:
channels_for_photons = [
ch for ch in channels_for_photons if ch != 0
]
if c.get('magically_avoid_dead_pmts', False):
channels_for_photons = [
ch for ch in channels_for_photons if c['gains'][ch] > 0
]
if c.get('magically_avoid_s1_excluded_pmts', False) and \
'channels_excluded_for_s1' in c:
channels_for_photons = [
ch for ch in channels_for_photons
if ch not in c['channels_excluded_for_s1']
]
c['channels_for_photons'] = channels_for_photons
# Determine sensible length of a pmt pulse to simulate
dt = c['sample_duration']
if c['pe_pulse_model'] == 'exponential':
c['samples_before_pulse_center'] = math.ceil(
c['pulse_width_cutoff'] * c['pmt_rise_time'] / dt)
c['samples_after_pulse_center'] = math.ceil(
c['pulse_width_cutoff'] * c['pmt_fall_time'] / dt)
else:
# Build the custom PMT pulse model
ts = np.array(c['pe_pulse_ts'])
ys = np.array(c['pe_pulse_ys'])
# Integrate and normalize it
# Note we're storing the integrated pulse, while the user gives the regular pulse.
c['pe_pulse_function'] = interp1d(ts,
np.cumsum(ys) / np.sum(ys),
bounds_error=False,
fill_value=(0, 1))
log.debug(
'Simulating %s samples before and %s samples after PMT pulse centers.'
% (c['samples_before_pulse_center'],
c['samples_after_pulse_center']))
# Load real noise data from file, if requested
if c['real_noise_file']:
self.noise_data = np.load(
utils.data_file_name(c['real_noise_file']))['arr_0']
# The silly XENON100 PMT offset again: it's relevant for indexing the array of noise data
# (which is one row per channel)
self.channel_offset = 1 if c['pmt_0_is_fake'] else 0
# Load light yields
self.s1_light_yield_map = InterpolatingMap(
utils.data_file_name(c['s1_light_yield_map']))
self.s2_light_yield_map = InterpolatingMap(
utils.data_file_name(c['s2_light_yield_map']))
# Load transverse field (r,z) distortion map
if c.get('rz_position_distortion_map'):
self.rz_position_distortion_map = InterpolatingMap(
utils.data_file_name(c['rz_position_distortion_map']))
else:
self.rz_position_distortion_map = None
# Init s2 per pmt lce map
qes = np.array(c['quantum_efficiencies'])
if c.get('s2_patterns_file', None) is not None:
self.s2_patterns = PatternFitter(
filename=utils.data_file_name(c['s2_patterns_file']),
zoom_factor=c.get('s2_patterns_zoom_factor', 1),
adjust_to_qe=qes[c['channels_top']],
default_errors=c['relative_qe_error'] +
c['relative_gain_error'])
else:
self.s2_patterns = None
##
# Load pdf for single photoelectron, if available
##
if c.get('photon_area_distribution'):
# Extract the spe pdf from a csv file into a pandas dataframe
spe_shapes = pd.read_csv(
utils.data_file_name(c['photon_area_distribution']))
# Create a converter array from uniform random numbers to SPE gains (one interpolator per channel)
# Scale the distributions so that they have an SPE mean of 1 and then calculate the cdf
# We have set the distribution of the off channels to be explicitly 0 as a precaution
# as of now these channels are
# 1, 2, 12, 26, 34, 62, 65, 79, 86, 88, 102, 118, 130, 134, 135, 139,
# 148, 150, 152, 162, 178, 183, 190, 198, 206, 213, 214, 234, 239, 244
uniform_to_pe_arr = []
for ch in spe_shapes.columns[
1:]: # skip the first element which is the 'charge' header
if spe_shapes[ch].sum() > 0:
mean_spe = (spe_shapes['charge'] *
spe_shapes[ch]).sum() / spe_shapes[ch].sum()
scaled_bins = spe_shapes['charge'] / mean_spe
cdf = np.cumsum(spe_shapes[ch]) / np.sum(spe_shapes[ch])
else:
# if sum is 0, just make some dummy axes to pass to interpolator
cdf = np.linspace(0, 1, 10)
scaled_bins = np.zeros_like(cdf)
uniform_to_pe_arr.append(interp1d(cdf, scaled_bins))
if uniform_to_pe_arr != []:
self.uniform_to_pe_arr = np.array(uniform_to_pe_arr)
else:
self.uniform_to_pe_arr = None
else:
self.uniform_to_pe_arr = None
# Init s1 pattern maps
# We're assuming the map is MC-derived, so we adjust for QE (just like for the S2 maps)
log.debug("Initializing s1 patterns...")
if c.get('s1_patterns_file', None) is not None:
self.s1_patterns = PatternFitter(
filename=utils.data_file_name(c['s1_patterns_file']),
zoom_factor=c.get('s1_patterns_zoom_factor', 1),
adjust_to_qe=qes[c['channels_in_detector']['tpc']],
default_errors=c['relative_qe_error'] +
c['relative_gain_error'])
else:
self.s1_patterns = None
##
# Luminescence time distribution precomputation
##
# For which gas gaps do we have to compute the luminescence time distribution?
gas_gap_warping_map = c.get('gas_gap_warping_map', None)
base_dg = c['elr_gas_gap_length']
if gas_gap_warping_map is not None:
with open(utils.data_file_name(gas_gap_warping_map),
mode='rb') as infile:
mh = pickle.load(infile)
self.gas_gap_length = lambda x, y: base_dg + mh.lookup([x], [y]
).item()
self.luminescence_converters_dgs = np.linspace(
mh.histogram.min(), mh.histogram.max(),
c.get('n_luminescence_time_converters', 20)) + base_dg
else:
self.gas_gap_length = lambda x, y: base_dg
self.luminescence_converters_dgs = np.array([base_dg])
self.luminescence_converters = []
# Calculate particle number density in the gas (ideal gas law)
number_density_gas = c['pressure'] / (units.boltzmannConstant *
c['temperature'])
# Slope of the drift velocity vs field relation
alpha = c['gas_drift_velocity_slope'] / number_density_gas
@np.vectorize
def yield_per_dr(E):
# Gives something proportional to the yield, not the yield itself!
y = E / (units.kV / units.cm) - 0.8 * c['pressure'] / units.bar
return max(y, 0)
rA = c['anode_field_domination_distance']
rW = c['anode_wire_radius']
for dg in self.luminescence_converters_dgs:
dl = c['gate_to_anode_distance'] - dg
rL = dg
# Voltage over the gas gap
V = c['anode_voltage'] / (
1 + dl / dg / c['lxe_dielectric_constant']
) # From eq1 in se note, * dg
# Field in the gas gap. r is distance from anode center: start at r=rL
E0 = V / (rL - rA + rA * (np.log(rA) - np.log(rW)))
@np.vectorize
def Er(r):
if r < rW:
return 0
elif rW <= r < rA:
return E0 * rA / r
else:
return E0
# Small numeric calculation to get emission time cdf
R = np.linspace(rL, rW, 1000)
E = Er(R)
RDOT = alpha * E
T = np.cumsum(-np.diff(R)[0] / RDOT) # dt = dx / v
yield_density = yield_per_dr(
E) * RDOT # density/dt = density/dx * dx/dt
yield_density /= yield_density.sum()
# Invert CDF using interpolator
uniform_to_emission_time = interp1d(np.cumsum(yield_density),
T,
fill_value=0,
bounds_error=False)
self.luminescence_converters.append(uniform_to_emission_time)
self.clear_signals_queue()
def startup(self):
aftmap_filename = utils.data_file_name(
'XENON1T_s1_aft_xyz_20170808.json')
self.aft_map = InterpolatingMap(aftmap_filename)
def __init__(self, config_to_init):
c = self.config = config_to_init
# Should we repeat events?
if 'event_repetitions' not in c:
c['event_repetitions'] = 1
# Primary excimer fraction from Nest Version 098
# See G4S1Light.cc line 298
density = c['liquid_density'] / (units.g / units.cm ** 3)
excfrac = 0.4 - 0.11131 * density - 0.0026651 * density ** 2 # primary / secondary excimers
excfrac = 1 / (1 + excfrac) # primary / all excimers
# primary / all excimers that produce a photon:
excfrac /= 1 - (1 - excfrac) * (1 - c['s1_ER_recombination_fraction'])
c['s1_ER_primary_excimer_fraction'] = excfrac
log.debug('Inferred s1_ER_primary_excimer_fraction %s' % excfrac)
# Recombination time from NEST 2014
# 3.5 seems fishy, they fit an exponential to data, but in the code they use a non-exponential distribution...
efield = (c['drift_field'] / (units.V / units.cm))
c['s1_ER_recombination_time'] = 3.5 / 0.18 * (1 / 20 + 0.41) * math.exp(-0.009 * efield)
log.debug('Inferred s1_ER_recombination_time %s ns' % c['s1_ER_recombination_time'])
# Which channels stand to receive any photons?
channels_for_photons = c['channels_in_detector']['tpc']
if c['pmt_0_is_fake']:
channels_for_photons = [ch for ch in channels_for_photons if ch != 0]
if c.get('magically_avoid_dead_pmts', False):
channels_for_photons = [ch for ch in channels_for_photons if c['gains'][ch] > 0]
if c.get('magically_avoid_s1_excluded_pmts', False) and \
'channels_excluded_for_s1' in c:
channels_for_photons = [ch for ch in channels_for_photons
if ch not in c['channels_excluded_for_s1']]
c['channels_for_photons'] = channels_for_photons
# Determine sensible length of a pmt pulse to simulate
dt = c['sample_duration']
if c['pe_pulse_model'] == 'exponential':
c['samples_before_pulse_center'] = math.ceil(c['pulse_width_cutoff'] * c['pmt_rise_time'] / dt)
c['samples_after_pulse_center'] = math.ceil(c['pulse_width_cutoff'] * c['pmt_fall_time'] / dt)
else:
# Build the custom PMT pulse model
ts = np.array(c['pe_pulse_ts'])
ys = np.array(c['pe_pulse_ys'])
# Integrate and normalize it
# Note we're storing the integrated pulse, while the user gives the regular pulse.
c['pe_pulse_function'] = interp1d(ts, np.cumsum(ys)/np.sum(ys), bounds_error=False, fill_value=(0, 1))
log.debug('Simulating %s samples before and %s samples after PMT pulse centers.' % (
c['samples_before_pulse_center'], c['samples_after_pulse_center']))
# Load real noise data from file, if requested
if c['real_noise_file']:
self.noise_data = np.load(utils.data_file_name(c['real_noise_file']))['arr_0']
# The silly XENON100 PMT offset again: it's relevant for indexing the array of noise data
# (which is one row per channel)
self.channel_offset = 1 if c['pmt_0_is_fake'] else 0
# Load light yields
self.s1_light_yield_map = InterpolatingMap(utils.data_file_name(c['s1_light_yield_map']))
self.s2_light_yield_map = InterpolatingMap(utils.data_file_name(c['s2_light_yield_map']))
# Load transverse field (r,z) distortion map
if c.get('rz_position_distortion_map'):
self.rz_position_distortion_map = InterpolatingMap(utils.data_file_name(c['rz_position_distortion_map']))
else:
self.rz_position_distortion_map = None
# Init s2 per pmt lce map
qes = np.array(c['quantum_efficiencies'])
if c.get('s2_patterns_file', None) is not None:
self.s2_patterns = PatternFitter(filename=utils.data_file_name(c['s2_patterns_file']),
zoom_factor=c.get('s2_patterns_zoom_factor', 1),
adjust_to_qe=qes[c['channels_top']],
default_errors=c['relative_qe_error'] + c['relative_gain_error'])
else:
self.s2_patterns = None
##
# Load pdf for single photoelectron, if available
##
if c.get('photon_area_distribution'):
# Extract the spe pdf from a csv file into a pandas dataframe
spe_shapes = pd.read_csv(utils.data_file_name(c['photon_area_distribution']))
# Create a converter array from uniform random numbers to SPE gains (one interpolator per channel)
# Scale the distributions so that they have an SPE mean of 1 and then calculate the cdf
# We have set the distribution of the off channels to be explicitly 0 as a precaution
# as of now these channels are
# 1, 2, 12, 26, 34, 62, 65, 79, 86, 88, 102, 118, 130, 134, 135, 139,
# 148, 150, 152, 162, 178, 183, 190, 198, 206, 213, 214, 234, 239, 244
uniform_to_pe_arr = []
for ch in spe_shapes.columns[1:]: # skip the first element which is the 'charge' header
if spe_shapes[ch].sum() > 0:
mean_spe = (spe_shapes['charge'] * spe_shapes[ch]).sum() / spe_shapes[ch].sum()
scaled_bins = spe_shapes['charge'] / mean_spe
cdf = np.cumsum(spe_shapes[ch])/np.sum(spe_shapes[ch])
else:
# if sum is 0, just make some dummy axes to pass to interpolator
cdf = np.linspace(0, 1, 10)
scaled_bins = np.zeros_like(cdf)
uniform_to_pe_arr.append(interp1d(cdf, scaled_bins))
if uniform_to_pe_arr != []:
self.uniform_to_pe_arr = np.array(uniform_to_pe_arr)
else:
self.uniform_to_pe_arr = None
else:
self.uniform_to_pe_arr = None
# Init s1 pattern maps
# We're assuming the map is MC-derived, so we adjust for QE (just like for the S2 maps)
log.debug("Initializing s1 patterns...")
if c.get('s1_patterns_file', None) is not None:
self.s1_patterns = PatternFitter(filename=utils.data_file_name(c['s1_patterns_file']),
zoom_factor=c.get('s1_patterns_zoom_factor', 1),
adjust_to_qe=qes[c['channels_in_detector']['tpc']],
default_errors=c['relative_qe_error'] + c['relative_gain_error'])
else:
self.s1_patterns = None
##
# Luminescence time distribution precomputation
##
# For which gas gaps do we have to compute the luminescence time distribution?
gas_gap_warping_map = c.get('gas_gap_warping_map', None)
base_dg = c['elr_gas_gap_length']
if gas_gap_warping_map is not None:
with open(utils.data_file_name(gas_gap_warping_map), mode='rb') as infile:
mh = pickle.load(infile)
self.gas_gap_length = lambda x, y: base_dg + mh.lookup([x], [y]).item()
self.luminescence_converters_dgs = np.linspace(mh.histogram.min(),
mh.histogram.max(),
c.get('n_luminescence_time_converters', 20)) + base_dg
else:
self.gas_gap_length = lambda x, y: base_dg
self.luminescence_converters_dgs = np.array([base_dg])
self.luminescence_converters = []
# Calculate particle number density in the gas (ideal gas law)
number_density_gas = c['pressure'] / (units.boltzmannConstant * c['temperature'])
# Slope of the drift velocity vs field relation
alpha = c['gas_drift_velocity_slope'] / number_density_gas
@np.vectorize
def yield_per_dr(E):
# Gives something proportional to the yield, not the yield itself!
y = E / (units.kV / units.cm) - 0.8 * c['pressure'] / units.bar
return max(y, 0)
rA = c['anode_field_domination_distance']
rW = c['anode_wire_radius']
for dg in self.luminescence_converters_dgs:
dl = c['gate_to_anode_distance'] - dg
rL = dg
# Voltage over the gas gap
V = c['anode_voltage'] / (1 + dl/dg/c['lxe_dielectric_constant']) # From eq1 in se note, * dg
# Field in the gas gap. r is distance from anode center: start at r=rL
E0 = V/(rL - rA + rA * (np.log(rA) - np.log(rW)))
@np.vectorize
def Er(r):
if r < rW:
return 0
elif rW <= r < rA:
return E0 * rA / r
else:
return E0
# Small numeric calculation to get emission time cdf
R = np.linspace(rL, rW, 1000)
E = Er(R)
RDOT = alpha * E
T = np.cumsum(- np.diff(R)[0] / RDOT) # dt = dx / v
yield_density = yield_per_dr(E) * RDOT # density/dt = density/dx * dx/dt
yield_density /= yield_density.sum()
# Invert CDF using interpolator
uniform_to_emission_time = interp1d(np.cumsum(yield_density), T,
fill_value=0, bounds_error=False)
self.luminescence_converters.append(uniform_to_emission_time)
self.clear_signals_queue()
def startup(self):
aftmap_filename = utils.data_file_name(
's1_aft_xyz_XENON1T_06Mar2017.json')
self.aft_map = InterpolatingMap(aftmap_filename)
self.low_pe_threshold = 10 # below this in PE, transition to hits
