| 1 | /* ======================================================================== *\
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| 2 | !
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| 3 | ! *
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| 4 | ! * This file is part of MARS, the MAGIC Analysis and Reconstruction
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| 5 | ! * Software. It is distributed to you in the hope that it can be a useful
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| 6 | ! * and timesaving tool in analysing Data of imaging Cerenkov telescopes.
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| 7 | ! * It is distributed WITHOUT ANY WARRANTY.
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| 8 | ! *
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| 9 | ! * Permission to use, copy, modify and distribute this software and its
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| 10 | ! * documentation for any purpose is hereby granted without fee,
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| 11 | ! * provided that the above copyright notice appear in all copies and
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| 12 | ! * that both that copyright notice and this permission notice appear
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| 13 | ! * in supporting documentation. It is provided "as is" without express
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| 14 | ! * or implied warranty.
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| 15 | ! *
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| 16 | !
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| 17 | !
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| 18 | ! Author(s): Markus Gaug 02/2004 <mailto:markus@ifae.es>
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| 19 | !
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| 20 | ! Copyright: MAGIC Software Development, 2000-2004
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| 21 | !
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| 22 | !
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| 23 | \* ======================================================================== */
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| 24 |
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| 25 | /////////////////////////////////////////////////////////////////////////////
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| 26 | // //
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| 27 | // MCalibrationChargePix //
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| 28 | // //
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| 29 | // Storage container of the calibrated Quantrum Efficiency of one pixel
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| 30 | // For the moment, only a fixed average QE is stored:
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| 31 | //
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| 32 | // - Average QE: (email David Paneque, 14.2.04):
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| 33 | //
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| 34 | // The conversion factor that comes purely from QE folded to a Cherenkov
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| 35 | // spectrum has to be multiplied by:
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| 36 | // * Plexiglass window -->> 0.96 X 0.96
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| 37 | // * PMT photoelectron collection efficiency -->> 0.9
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| 38 | // * Light guides efficiency -->> 0.94
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| 39 | //
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| 40 | // Concerning the light guides effiency estimation... Daniel Ferenc
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| 41 | // is preparing some work (simulations) to estimate it. Yet so far, he has
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| 42 | // been busy with other stuff, and this work is still UNfinished.
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| 43 | //
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| 44 | // The estimation I did comes from:
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| 45 | // 1) Reflectivity of light guide walls is 85 % (aluminum)
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| 46 | // 2) At ZERO degree light incidence, 37% of the light hits such walls
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| 47 | // (0.15X37%= 5.6% of light lost)
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| 48 | // 3) When increasing the light incidence angle, more and more light hits
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| 49 | // the walls.
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| 50 | //
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| 51 | // However, the loses due to larger amount of photons hitting the walls is more
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| 52 | // or less counteracted by the fact that more and more photon trajectories cross
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| 53 | // the PMT photocathode twice, increasing the effective sensitivity of the PMT.
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| 54 | //
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| 55 | // Jurgen Gebauer did some quick measurements about this issue. I attach a
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| 56 | // plot. You can see that the angular dependence is (more or less) in agreement
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| 57 | // with a CosTheta function (below 20-25 degrees),
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| 58 | // which is the variation of teh entrance window cross section. So, in
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| 59 | // first approximation, no loses when increasing light incidence angle;
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| 60 | // and therefore, the factor 0.94.
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| 61 | //
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| 62 | // So, summarizing... I would propose the following conversion factors
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| 63 | // (while working with CT1 cal box) in order to get the final number of photons
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| 64 | // from the detected measured size in ADC counts.
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| 65 | //
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| 66 | // Nph = ADC * FmethodConversionFactor / ConvPhe-PhFactor
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| 67 | //
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| 68 | // FmethodConversionFactor ; measured for individual pmts
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| 69 | //
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| 70 | // ConvPhe-PhFactor = 0.98 * 0.23 * 0.90 * 0.94 * 0.96 * 0.96 = 0.18
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| 71 | //
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| 72 | // I would not apply any smearing of this factor (which we have in nature),
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| 73 | // since we might be applying it to PMTs in the totally wrong direction.
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| 74 | //
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| 75 | //
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| 76 | /////////////////////////////////////////////////////////////////////////////
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| 77 | #include "MCalibrationQEPix.h"
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| 78 |
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| 79 | #include "MLog.h"
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| 80 | #include "MLogManip.h"
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| 81 |
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| 82 | ClassImp(MCalibrationQEPix);
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| 83 |
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| 84 | using namespace std;
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| 85 |
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| 86 | // --------------------------------------------------------------------------
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| 87 | //
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| 88 | // Default Constructor:
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| 89 | //
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| 90 | MCalibrationQEPix::MCalibrationQEPix(const char *name, const char *title)
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| 91 | : fPixId(-1)
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| 92 | {
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| 93 |
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| 94 | fName = name ? name : "MCalibrationQEPix";
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| 95 | fTitle = title ? title : "Container of the calibrated quantum efficiency ";
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| 96 |
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| 97 | Clear();
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| 98 |
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| 99 | }
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| 100 |
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| 101 | // ------------------------------------------------------------------------
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| 102 | //
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| 103 | // Invalidate values
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| 104 | //
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| 105 | void MCalibrationQEPix::Clear(Option_t *o)
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| 106 | {
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| 107 |
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| 108 | SetExcluded ( kFALSE );
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| 109 | SetQEValid ( kFALSE );
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| 110 |
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| 111 | fQEGreen = -1.;
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| 112 | fQEBlue = -1.;
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| 113 | fQEUV = -1.;
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| 114 | fQECT1 = -1.;
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| 115 |
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| 116 | fQEGreenErr = -1.;
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| 117 | fQEBlueErr = -1.;
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| 118 | fQEUVErr = -1.;
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| 119 | fQECT1Err = -1.;
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| 120 |
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| 121 | }
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| 122 |
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| 123 |
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| 124 | void MCalibrationQEPix::SetQE( const Float_t qe, const PulserColor_t col )
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| 125 | {
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| 126 |
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| 127 | switch (col)
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| 128 | {
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| 129 | case kGREEN:
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| 130 | fQEGreen = qe;
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| 131 | break;
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| 132 | case kBLUE:
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| 133 | fQEBlue = qe;
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| 134 | break;
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| 135 | case kUV:
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| 136 | fQEUV = qe;
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| 137 | break;
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| 138 | case kCT1:
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| 139 | fQECT1 = qe;
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| 140 | break;
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| 141 | default:
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| 142 | fQECT1 = qe;
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| 143 | break;
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| 144 | }
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| 145 | }
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| 146 |
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| 147 | void MCalibrationQEPix::SetQEErr( const Float_t qeerr, const PulserColor_t col )
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| 148 | {
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| 149 |
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| 150 | switch (col)
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| 151 | {
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| 152 | case kGREEN:
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| 153 | fQEGreenErr = qeerr;
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| 154 | break;
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| 155 | case kBLUE:
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| 156 | fQEBlueErr = qeerr;
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| 157 | break;
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| 158 | case kUV:
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| 159 | fQEUVErr = qeerr;
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| 160 | break;
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| 161 | case kCT1:
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| 162 | fQECT1Err = qeerr;
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| 163 | break;
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| 164 | default:
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| 165 | fQECT1Err = qeerr;
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| 166 | break;
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| 167 | }
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| 168 | }
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| 169 |
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| 170 |
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| 171 |
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| 172 | // --------------------------------------------------------------------------
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| 173 | //
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| 174 | // Set the Excluded Bit from outside
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| 175 | //
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| 176 | void MCalibrationQEPix::SetExcluded(Bool_t b )
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| 177 | {
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| 178 | b ? SETBIT(fFlags, kExcluded) : CLRBIT(fFlags, kExcluded);
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| 179 | }
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| 180 |
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| 181 | // --------------------------------------------------------------------------
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| 182 | //
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| 183 | // Set the Excluded Bit from outside
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| 184 | //
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| 185 | void MCalibrationQEPix::SetQEValid(Bool_t b )
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| 186 | {
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| 187 | b ? SETBIT(fFlags, kQEValid) : CLRBIT(fFlags, kQEValid);
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| 188 | }
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| 189 |
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| 190 |
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| 191 | Int_t MCalibrationQEPix::GetPixId() const
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| 192 | {
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| 193 | return fPixId;
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| 194 | }
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| 195 |
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| 196 | Float_t MCalibrationQEPix::GetQE(const PulserColor_t col ) const
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| 197 | {
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| 198 |
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| 199 | switch (col)
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| 200 | {
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| 201 | case kGREEN:
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| 202 | return fQEGreen;
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| 203 | break;
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| 204 | case kBLUE:
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| 205 | return fQEBlue;
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| 206 | break;
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| 207 | case kUV:
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| 208 | return fQEUV;
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| 209 | break;
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| 210 | case kCT1:
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| 211 | return fQECT1;
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| 212 | break;
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| 213 | default:
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| 214 | return fQECT1;
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| 215 | break;
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| 216 | }
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| 217 | }
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| 218 |
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| 219 | Float_t MCalibrationQEPix::GetQEErr(const PulserColor_t col ) const
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| 220 | {
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| 221 |
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| 222 | switch (col)
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| 223 | {
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| 224 | case kGREEN:
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| 225 | return fQEGreenErr;
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| 226 | break;
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| 227 | case kBLUE:
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| 228 | return fQEBlueErr;
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| 229 | break;
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| 230 | case kUV:
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| 231 | return fQEUVErr;
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| 232 | break;
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| 233 | case kCT1:
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| 234 | return fQECT1Err;
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| 235 | break;
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| 236 | default:
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| 237 | return fQECT1Err;
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| 238 | break;
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| 239 | }
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| 240 | }
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| 241 |
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| 242 |
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| 243 | Bool_t MCalibrationQEPix::IsExcluded() const
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| 244 | {
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| 245 | return TESTBIT(fFlags,kExcluded);
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| 246 | }
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| 247 |
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| 248 |
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| 249 | Bool_t MCalibrationQEPix::IsQEValid() const
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| 250 | {
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| 251 | return TESTBIT(fFlags, kQEValid);
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| 252 | }
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| 253 |
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| 254 |
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| 255 | //
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| 256 | // The check return kTRUE if:
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| 257 | //
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| 258 | // 1) Pixel has a fitted charge greater than fQELimit*PedRMS
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| 259 | // 2) Pixel has a fit error greater than fQEErrLimit
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| 260 | // 3) Pixel has a fitted charge greater its fQERelErrLimit times its charge error
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| 261 | // 4) Pixel has a charge sigma bigger than its Pedestal RMS
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| 262 | //
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| 263 | Bool_t MCalibrationQEPix::CheckQEValidity()
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| 264 | {
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| 265 |
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| 266 | SetQEValid();
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| 267 | return kTRUE;
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| 268 | }
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