55 reconstructor( reconstructor_ ), useTableMass( NULL ),
56 useMassCut( NULL ), mCutOPCenter( NULL ), mCutNOPCenter( NULL ),
57 mCutOPWidth( NULL ), mCutNOPWidth( NULL ), mCutAngle( NULL ),
58 useAbsorbedEnergyCut( NULL ), aeCutCLCenter( NULL ),
59 aeCutCRCenter( NULL ), aeCutCLWidth( NULL ), aeCutCRWidth( NULL ),
60 aeCutAngle( NULL ), setExpectedMomentumAmp( NULL ),
61 setExpectedMomentumAmpDiff( NULL ), setEDCollectionAlgorithm( NULL )
67 "table mass of output\n particle when building output particle "
68 "energy,\n otherwise reconstructed mass will be used" );
76 "particle\n and nucleus output particle" );
88 outputParticle->GetPDGMass() );
97 "particle mass\n coordinate" );
100 nucleusOutputParticle->GetPDGMass() );
112 outputParticle->GetPDGMass() * 0.1 );
121 "particle mass\n coordinate" );
124 nucleusOutputParticle->GetPDGMass() * 0.1 );
143 "energies in\n calorimeters" );
152 "calorimeter\n absorbed energy coordinate" );
163 "calorimeter\n absorbed energy coordinate" );
174 "\n absorbed energy coordinate" );
185 "\n absorbed energy coordinate" );
206 "expected in the target;\n this value may differ from original "
207 "momentum\n of the beam as far as profile data of the beam refer\n"
208 " to the place where it starts. This parameter is used only\n"
209 " in reconstruction procedure");
220 "between momenta of the beam\n on its start and in the target. This "
221 "parameter can\n be used to automatically calculate value of the\n"
222 " previous parameter 'momentumAmp'" );
234 "\n Choose crystals to be selected when energy deposit collected\n"
236 " adjacent - crystal with maximum energy deposit and\n"
237 " adjacent crystals" );
369 if ( value ==
"adjacent" )