1 | #!/usr/bin/python -tti
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2 | #
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3 | # calculation of DRS Time Calibration constants
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4 | # initial implementation by Remo Dietlicher and Werner Lustermann (ETH Zurich)
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5 | # based on C++ classes by Oliver Grimm (ETH Zurich)
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6 | #
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7 | # this python implementation was coded by
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8 | # D. Neise (TU Dortmund) April 2012
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9 | #
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10 | import numpy as np
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11 | from pyfact import RawData
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12 | from drs_spikes import DRSSpikes
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13 | from extractor import ZeroXing
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14 | class CalculateDrsTimeCalibrationConstants( object ):
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15 | """ basic analysis class for the calculation of DRS time aperture jitter calibration constants
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16 | """
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17 |
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18 | def __init__(self, dpath, cpath):
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19 | """
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20 | *dpath*: data file path, file should contain a periodic signal in eahc 9th channel
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21 | *cpath*: std DRS amplitude calibration path
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22 | """
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23 | #dfname = '/data00/fact-construction/raw/2011/11/24/20111124_113.fits.gz'
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24 | #calfname = '/data00/fact-construction/raw/2011/11/24/20111124_111.drs.fits.gz'
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25 | self.data_path = dpath
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26 | self.calib_path = cpath
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27 | self.run = RawData(dpath, cpath, return_dict = True)
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28 |
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29 | if self.run.nroi != 1024:
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30 | raise TypeError('Time Calibration Data must have ROI=1024, ROI of '+dpath+' is: '+str(self.run.nroi))
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31 |
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32 | self.despike = DRSSpikes()
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33 | self.zero_crossing_finder = ZeroXing(slope = -1) # -1 means falling edge
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34 | self.fsampling = 2. # sampling frequency
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35 | self.freq = 250. # testfrequency
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36 | self.P_nom = 1000./self.freq # nominal Period due to testfrequency
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37 | self.DAMPING = 0.02 # Damping applied to correction
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38 |
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39 | # this ndarray will contain the best estimate of the true width of each slice after a __call__
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40 | # but it is used to determine the current best estimate inside the __call__ as well,
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41 | # since the algorithm is iteratively implemented
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42 | #self.time_calib = np.linspace( 0. , 512, num=1024, endpoint=False).repeat(run.npix/9).reshape( (1024,run.npix/9) ).transpose()
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43 | self.time_calib = np.ones( (self.run.npix/9, 1024) )/self.fsampling
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44 | def __call__(self):
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45 | """ the class-call method performs the actual calculation based on the input data
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46 | returns: tuple of length 160 containing tuples of length 1024 containing the length of each cell in ns
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47 | the class contains self.result after the call.
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48 | """
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49 | # loop over events
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50 | counter = 0
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51 | for event in self.run:
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52 | print 'counter', counter
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53 | counter +=1
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54 | # in the next() method, which is called during looping,
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55 | # the data is automatically amplitude calibrated.
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56 | # we just need every 9th pixel, so this is a place
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57 | # for optimization
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58 | data = event['acal_data']
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59 |
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60 | # slice out every 9th channel
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61 | niners_ids = range(8,self.run.npix,9) # [8, 17, 26, ..., 1430, 1439]
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62 | data = data[niners_ids,:]
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63 | start_cell = event['start_cells'][niners_ids,:]
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64 |
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65 | data = self.despike( data )
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66 |
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67 | # shift data down by the mean # possible in one line
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68 | # calculate mean
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69 | mean = data.mean(1)
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70 | # make mean in the same shape as data, for elementwise subtraction
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71 | mean = mean.repeat(data.shape[1]).reshape(data.shape)
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72 | # subtraction
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73 | data = data - mean
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74 |
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75 | # find zero crossings with falling edge
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76 | # the output is a list, of lists, of slices.
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77 | # each slice, shows a zero crossing. in fact, is is the slice where
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78 | # the data is still positive ... in the next slice it is negative, (or just zero).
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79 | # This was called 'MeanXing' before
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80 | all_crossings = self.zero_crossing_finder(data)
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81 |
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82 | # now we have to calculate the exact time of the crossings
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83 | # but in units of nanoseconds therefor we use self.time_calib
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84 | # rolled appropriately, and summed up in order to have the integral timing calibration
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85 | #
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86 | #the list, 'time_of_all_crossings' will contain sublists,
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87 | # which in turn will contain the times, in ns, for each zero-crossing
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88 | time_of_all_crossings = []
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89 | # the list, 'float_slice_of_all_crossings'
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90 | # is similar to the list above, but i just contains the position of the crossings
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91 | # in the pipeline, but more precisely than 'all_crossings', the position is linear interpolated
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92 | float_slice_of_all_crossings = []
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93 |
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94 | for chip_id,crossings in enumerate(all_crossings):
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95 | time_of_all_crossings.append([])
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96 | float_slice_of_all_crossings.append([])
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97 | time = np.roll(self.time_calib[chip_id], -start_cell[chip_id]).cumsum()
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98 | for crossing in crossings:
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99 | # performing linear interpolation of time of zero crossing
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100 | # what fraction of a slide is the interpolated crossing away from the integral slice id
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101 | fraction_of_slice = data[chip_id,crossing] / (data[chip_id,crossing]-data[chip_id,crossing+1])
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102 | float_slice_of_all_crossings[-1].append(fraction_of_slice + crossing)
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103 | slope = time[crossing+1] - time[crossing]
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104 | time_of_crossing = time[crossing] + slope * fraction_of_slice
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105 | time_of_all_crossings[-1].append(time_of_crossing)
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106 |
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107 | # Now one can use those two lists, which were just created
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108 | # to calculate the number(float) of slices between two consecutive crossings
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109 | # as well as the *measured* time between two crossings.
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110 | # on the other hand, the period of the test signal is known to be self.P_nom
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111 | # so in case the measured time is longer or shorter than the known Period
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112 | # the associated time of all involved slices
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113 | # is assumed to be a bit longer or short than 1./self.fsampling
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114 |
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115 | # first we make the sublists of the lists to be numpy.arrays
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116 | for i in range(len(float_slice_of_all_crossings)): #both list have equal length
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117 | float_slice_of_all_crossings[i] = np.array(float_slice_of_all_crossings[i])
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118 | time_of_all_crossings[i] = np.array(time_of_all_crossings[i])
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119 |
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120 | # now we can easily calculate the measured periods using np.diff()
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121 | all_measured_periods = []
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122 | for chip_times in time_of_all_crossings:
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123 | all_measured_periods.append(np.diff(chip_times))
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124 |
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125 | for chip,chip_periods in enumerate(all_measured_periods):
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126 |
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127 | for i,period in enumerate(chip_periods):
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128 | #shortcuts to the involved slices
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129 | start = all_crossings[chip][i]
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130 | end = all_crossings[chip][i+1]
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131 | interval = end-start
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132 | rest = 1024-interval
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133 |
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134 | delta_period = (self.P_nom - period) * self.DAMPING
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135 | # nominal_number_of_slices
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136 | nom_num_slices = period * self.fsampling
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137 |
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138 | # now the delta_period is distributed to all slices
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139 | # I do not exactly understand the +1 here ... error prone!!!
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140 | # the following explanation assumes delta_period is positive
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141 | # the slices between start and end get a positive correction value
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142 | # This correction value is given by delta_period / nom_num_slices
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143 | pos_fraction = delta_period / nom_num_slices
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144 | # the total positive correction sums up to
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145 | total_positive_correction = interval * pos_fraction
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146 | # the total negative correction must sum up to the sampe value
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147 | total_negative_correction = rest * (interval * (pos_fraction/rest))
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148 | # so we can call the product following 'rest' the 'neg_fraction
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149 | neg_fraction = -1 * interval/rest * pos_fraction
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150 | #print '1. should be zero', total_positive_correction - total_negative_correction
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151 | #assert total_positive_correction - total_negative_correction == 0
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152 |
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153 | correction = np.zeros(1024)
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154 | correction[start+1:end+1] = pos_fraction
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155 | correction[:start+1] = neg_fraction
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156 | correction[end+1:] = neg_fraction
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157 | #print '2. should be zero', correction.sum()
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158 | #assert correction.sum() == 0
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159 |
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160 | # now we have to add these correction values to self.time_calib
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161 | self.time_calib[chip,:] += np.roll(correction, start_cell[chip])
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