// MAUS WARNING: THIS IS LEGACY CODE. // @(#) $Id: dataCards.cc,v 1.307 2011-05-20 14:28:40 reid Exp $ $Name: $ /* ** modified from Yagmur Torun's MICE simulation package ** Ed McKigney - Aug 21 2002 */ #include #include "Interface/dataCards.hh" #include "Utils/Squeak.hh" #include "Utils/Exception.hh" #include "CLHEP/Units/SystemOfUnits.h" using CLHEP::ms; using CLHEP::mm; using CLHEP::ns; using CLHEP::MeV; using CLHEP::megahertz; using CLHEP::keV; using CLHEP::coulomb; using CLHEP::rad; using CLHEP::picosecond; using CLHEP::cm; #include #include #include #include using std::cout; using std::cin; using std::endl; using std::vector; dataCards::dataCards() { } std::string dataCards::getClient() { return client; } void dataCards::initializeApplicationCodes() { appCode["Simulation"] = 0; appCode["Digitization"] = 1; appCode["Reconstruction"] = 2; appCode["Analysis"] = 3; } dataCards::dataCards(const std::string& app) : client(app) { initializeApplicationCodes(); std::map::iterator i = appCode.find(client); if (i == appCode.end()) { throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Unrecognized client application for datacards", "dataCards(...)")); } fillCards(i->second); } dataCards::dataCards(int app) { fillCards(app); } void dataCards::AddDataCard( std::string aName, std::string aDefaultValue ){ cs[ aName ] = aDefaultValue; } void dataCards::AddDataCard( std::string aName, int aDefaultValue ){ ci[ aName ] = aDefaultValue; } void dataCards::AddDataCard( std::string aName, double aDefaultValue ){ cd[ aName ] = aDefaultValue; } void dataCards::AddDataCard( std::string aName, vector< double > aDefaultValue ){ cv[ aName ] = aDefaultValue; } void dataCards::AddDataCard( std::string aName, const unsigned int aSize, double * aDefaultValue ){ vector dVector; dVector.assign( aDefaultValue, aDefaultValue + aSize ); cv[ aName ] = dVector; } void dataCards::fillCards(int app) { if (app == 0) { // app = 0 for Simulation cs["OutputFile"] = "Sim.out.gz"; cs["InputFile"] = "none"; } else if (app == 1) { // app = 1 for Digitization cs["InputFile"] = "Sim.out.gz"; cs["OutputFile"] = "Digits.out.gz"; } else if (app == 2) { // app = 2 for Reconstruction cs["InputFile"] = "Digits.out.gz"; cs["OutputFile"] = "Rec.out.gz"; } else if (app == 3) { // app = 3 for Analysis cs["InputFile"] = "Rec.out.gz"; cs["OutputFile"] = "Ana.out"; } else { throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Unrecognized client application for datacards", "dataCards::fillCards")); } cs["FileTag"] = ""; //Can be used as a component of output filenames for various applications, being descriptive of the beam and analysis, e.g. 400MeVpions. Convenient for batch scripts. double QuadFringeParams[6] = {0.296471, 4.533219, -2.270982, 1.068627, -0.036391, 0.022261}; //THIS IS PUT UP HERE TO STOP IT INTERFERING WITH DOC SCRIPT //***Start Doc Script*** // Global run control ci["numEvts"] = 100; // Number of events in the run ci["runNumber"] = 1; // Run number listed in header of some output files cs["Description"] = "G4MICE events"; // Description of the run listed in the header of some output files cs["DataType"] = "TextFile"; //The data type of the dataCards file, set by user and used in global reader, TextFileReader etc // Modelling and Configuration cs["GeometrySchema"] = "http://service-spi.web.cern.ch/service-spi/app/releases/GDML/GDML_3_0_0/schema/gdml.xsd"; // GDML schema (built-in default will be used if not found) cs["ReadGeometryURL"] = "http://rgma19.pp.rl.ac.uk:8080/cdb/geometry"; // To be overridden cs["WriteGeometryURL"] = "http://rgma19.pp.rl.ac.uk:8080/cdb/geometrySuperMouse"; // ...so it can be different cs["GeometrySource"] = "MiceModelTextFile"; //Or "RunNumber", "CurrentGeometry", "GeometryID", "GDMLTextFile" cs["MiceModel"] = "MICEStage6/Stage6.dat"; // The MiceModel, as defined in $MICEFILES/Models/Configurations/ cs["SciFiCalib"] = ""; //SciFi detector calibration file, found in ${MICEFILES}/Calibration/ cs["TofCalib"] = "tofcalib"; //TOF detector calibration file, found in ${MICEFILES}/Calibration/ cs["SciFiCable"] = ""; //SciFi detector cabling file, found in ${MICEFILES}/Cabling/SciFi/ cs["SciFiCableType"] = ""; //Set to "Imperial" or "Osaka" for different cabling types cs["TofCable"] = "tofcabling.txt"; //Tof detector cabling file, found in ${MICEFILES}/Cabling/ ci["FieldGridX"] = 2; //Number of points in the field grid in x. As an optimisation, G4MICE divides the world into a grid. At each step, G4MICE only looks at fields in the local grid. The number of points in each dimension should roughly match the size of the problem in each dimension for a reasonable option, and FieldGridX*FieldGridY*FieldGridZ should be small, say<1e6. ci["FieldGridY"] = 2; //Number of points in the field grid in y ci["FieldGridZ"] = 100; //Number of points in the field grid in z // Simulation Application run control cd["MaxRadiusInChannel"] = 1.e9 * mm; // Events with r = sqrt(x^2 + y^2) > MaxRadius in global coordinates are killed cd["MaxZInChannel"] = 1.e9 * mm; // Events with z > MaxZ are killed in Simulation cd["MaxTimeAllowed"] = 1. * ms; // Events with t > MaxT are killed in Simulation ci["RandomSeed"] = 0; // Random seed for stochastic algorithms cs["PhysicsModel"] = "QGSP_BERT"; //Physics package loaded by G4MICE to set default values; modifications can be made as per following cs["MultipleScatteringModel"] = "mcs"; //"mcs" (multiple coulomb scattering) or "none" cs["EnergyLossModel"] = "estrag"; //"estrag" (full energy loss), "ionisation" (mean energy loss only) or "none" cs["HadronicModel"] = "All"; //"All" (All hadronic interactions) or "None" (no hadronic interactions) cs["MuonDecay"] = ""; //Deprecated; please use ParticleDecay datacard cs["ParticleDecay"] = "True"; //Set to "True" or "False" to determine whether muons decay cs["ReferenceEnergyLossModel"] = "ionisation"; //Energy loss model of reference particle; set to "none" or "ionisation". Reference particle can never have stochastic processes (e.g. estrag, mcs) enabled. cs["ReferenceG4UIScript"] = ""; //If a filename is given, G4MICE will run this as a macro to G4UI after setting up ReferenceEnergyLossModel but before firing the reference particle. Enables any extra set-up that may be required. cs["BeginOfRunG4UIScript"] = ""; //If a filename is given, G4MICE will run this as a macro to G4UI after firing the reference particle but before firing the beam. Enables any extra set-up that may be required. cs["EverythingSpecialVirtual"] = ""; //Set to "true" to make every physical volume a special virtual detector ci["WriteReferenceParticle"] = 0; // Set to 1 to write reference particle hits during simulation; or 0 to ignore them cd["ProductionThreshold"] = 0.5 * mm; //I *think* threshold for delta ray production cd["MuonHalfTime"] = -1 * ns; //Set the muon half life; use g4 default if negative. cd["ChargedPionHalfTime"] = -1 * ns; //Set the pi+ and pi- half life; use g4 default if negative. cs["TrackOnlyMuons"] = "False"; //Set to true to kill non-muons on production ci["MaxStepsWOELoss"] = 2000; //Maximum number of steps taken without energy loss - particles killed afterwards ci["StepStatisticsOutput"] = 0; //I *think* set to 1 to see physics processes output cs["StepStatisticsVolume"] = "All"; //I *think* selects which volumes to write physics processes output from ci["CheckVolumeOverlaps"] = 0; //Set to 1 to check for volume overlaps in GEANT4 physical volumes // Simulation Application beam control cs["BeamType"] = "Pencil"; //Type of beam; "Pencil" generates a pencil beam using parameters below, "Gaussian" generates a beam with gaussian distribution using parameters below, "ICOOL", "G4BeamLine", "TURTLE", "G4MICE_PrimaryGenHit" set G4MICE to read from a beam file with the appropriate format and file name defined in datacard "InputBeamFileName"; "MiceModule" uses the beam definition taken from MiceModules (see mice module docs), and allows arbitrary placement of beams with arbitrary multivariate gaussian distributions; in general, MiceModules are the preferred method for setting up beams. The reference particle is the first particle created. If BeamType is Random, the first particle will have no random distribution. cd["BeamMomentum"] = 200.0 * MeV; //When BeamType is Pencil or Random, controls momentum of the beam cd["ZOffsetStart"] = -6011. * mm; //Z-position of input beam when not in MiceModule mode. x and y are 0. Added to any z-position in beam file. ci["BeamPid"] = -13; //Particle ID of pencil beam and TURTLE beam (11 is e-, -13 is mu+, 211 is pi+, 2212 is proton) cs["InputBeamFileName"] = "none"; //Name of beam file for BeamTypes that use files, as specified in BeamType above cd["SigmaX"] = 0.*mm; //If beam type is "Gaussian", set RMS of x cd["SigmaXPrime"] = 0.; //If beam type is "Gaussian", set RMS of x' (px/p) cd["SigmaY"] = 0.*mm; //If beam type is "Gaussian", set RMS of y cd["SigmaYPrime"] = 0.; //If beam type is "Gaussian", set RMS of y' (py/p) cd["SigmaT"] = 0.*ns; //If beam type is "Gaussian", set RMS of time distribution cd["SigmaEOverE"] = 0.; //If beam type is "Gaussian", set RMS of (E-E_ref)/E_ref where E is total energy and E_ref is total energy corresponding to BeamMomentum // Beam Matcher Application Control cs["MatchAlgorithm"] = "EigenvalueSeed"; //The algorithm used for matching; "Eigenvalue" calculates the transfer map and then attempts to automatically derive the matched covariance matrix; "EigenvalueSeed" uses this automatic calculation as the seed for a numerical for a periodic solution, including e.g. some effects of material; "UserDefined" uses user input for the Twiss parameters at the LatticeStart; "UserDefinedSeed" uses user input for the seed Twiss parameters, and then iterates through an optimisation algorithm to find a periodic solution. cd["NormalisedCanonicalAngularMomentum"] = 0; //Normalised canonical angular momentum of beam at lattice start cd["LatticeStart"] = -2750 * mm; //Start of lattice over which beta is periodic cd["LatticeEnd"] = 2750 * mm; //End of lattice over which beta is periodic cd["EnergyAtLatticeStart"] = 226 * MeV; //Desired energy at start of the lattice cd["AlphaBetaScaleFactor"] = 11/0.05; //Weighting factor between alpha and beta for "Seed" algorithms cd["TransverseEmittance"] = 6 * mm; //Transverse emittance of generated beam cd["LongitudinalEmittance"] = 0.1 * ns; //Longitudinal emittance of generated beam cd["AmplitudeMomentumCorrelation"] = 0.; //amplitude momentum correlation introduces factor like p *= (1+(A-)*corr) to matched beam ci["NumberOfEnergyCoordinates"] = 1; // Calculate matched beta function for various energies cd["EnergyRange"] = 0. * MeV; // full energy range over which the multiple beta functions will be calculated cd["LongitudinalBeta"] = 10.; //longitudinal beta at z = LatticeStart; set to < 0. to auto-detect cd["LongitudinalAlpha"] = 0.; //longitudinal alpha at z = LatticeStart; only used if auto-detect is off cd["TransverseBeta"] = 420. * mm; //transverse beta at z = LatticeStart; set to < 0. to auto-detect cd["TransverseAlpha"] = 0.; //transverse alpha at z = LatticeStart; only used if auto-detect is off cd["DispersionX"] = 0. * mm; //Future development: x dispersion at z = LatticeStart for matcher cd["DispersionY"] = 0. * mm; //Future development: y dispersion at z = LatticeStart for matcher // Solenoids Field Controls cs["FieldMode"] = "Full"; //"Full" = use G4MICE field definitions; "Constant" = use G4 constant fields cs["SolDataFiles"] = "Write"; //"Write" = write solenoid field maps; "Read" = read solenoid field maps ci["NumberNodesZGrid"] = 100; //Default number of nodes in Z in the solenoid field map grid ci["NumberNodesRGrid"] = 150; //Default number of nodes in R in the solenoid field map grid cd["SolzMapExtendFactor"] = 10.0; // Set the Z extent of the solenoid field maps; z_extent of the field map = coil_length + z_factor*coil_inner_radius cd["SolrMapExtendFactor"] = 2.01828182845905; // Set the radial extent of solenoid field maps; r_extent of the field map = r_factor * coil_inner_radius ci["DefaultNumberOfSheets"] = 10; // number of sheets for solenoids. // Quadrupole Field Controls cd["QuadrupoleFringeMaxZFactor"] = 5.; //Maximum z extent of quadrupole fringe fields (as a fraction of quad length) ci["QuadrupoleUseFringeFields"] = 1; //Set to 1 to use fringe fields in quadrupoles fillVector("QuadrupoleFringeParameters",6,QuadFringeParams); /*comment below is included for documentation - don't delete*/ // double QuadFringeParams[6] = {0.296471, 4.533219, -2.270982, 1.068627, -0.036391, 0.022261}; //Default parameters for Enge function, that controls multipole fringe fields // RF Cavity Field Controls cd["rfAccelerationPhase"] = 1.57 * rad; //Default RF phase of all cavities. May go buggy if this is > pi/2 so be careful cd["OpticsRfFrequency"] = 201.25 * megahertz; //Global RF frequency assumed by optics module. cd["PhaseTolerance"] = 1e-5 * ns; //Tolerance on RF phase cd["RFDeltaEnergyTolerance"] = 1e-5 * MeV; //Tolerance on RF energy gain (peak field) //Simulation Application stepping parameters /*See G4 Docs on ElectroMagnetic fields*/ cd["DeltaOneStep"] = 1. * mm; // Estimate of error in end point in free space cd["DeltaIntersection"] = 1.e-3 * mm; // Estimate of error in step end point when a track intersects a new physical volume cd["EpsilonMin"] = 1.e-10 * mm; // Minimum on DeltaOneStep? (unclear in G4 docs) cd["EpsilonMax"] = 1.e+10 * mm; // Maximum on DeltaOneStep? (unclear in G4 docs) cd["MissDistance"] = 1.e-2 * mm; // Maximum miss distance when a track passes near a physical volume cs["FieldTrackStepper"] = "Classic"; // Set the integration algorithm for tracking. Options are for electromagnetic: "Classic" (= "ClassicalRK4"); "SimpleHeum"; "ImplicitEuler"; "SimpleRunge"; "ExplicitEuler"; and for magnetic only: "CashKarpRKF45"; "HelixImplicitEuler"; "HelixHeum"; "HelixSimpleRunge"; "HelixExplicitEuler". see G4 documentation for further details. cd["VirtualRelativeError"] = 1.e-4; //Relative error for virtual detector stepping cd["VirtualAbsoluteError"] = 1.e-4; //Absolute error for virtual detector stepping cd["MaxStepSizeInChannel"] = 10000.0 * mm; //Deprecated - does nothing // Simulation Application RF induced background controls - Deprecated do not use cs["rfBGMode"] = "none"; //Deprecated - does nothing cs["rfBGSource"] = "none"; //Deprecated - does nothing cs["rfBGElectronModel"] = "Simple"; //Deprecated - does nothing cs["rfBGPhotonModel"] = "Uniform"; //Deprecated - does nothing cs["rfBGEmitterMode"] = "Random"; //Deprecated - does nothing ci["rfBGNumberOfEmitters"] = 10; //Deprecated - does nothing ci["rfBGNumberOfElectrons"] = 1; //Deprecated - does nothing ci["rfBGNumberOfPhotons"] = 1; //Deprecated - does nothing ci["rfBGDirection"] = 0; //Deprecated - does nothing cd["rfBGElectronEnergy"] = .01 * MeV; //Deprecated - does nothing cd["rfBGPhotonEnergy"] = .1 * MeV; //Deprecated - does nothing cd["rfBGElectronEnergyWidth"] = .001 * MeV; //Deprecated - does nothing cd["rfBGPhotonEnergyWidth"] = .01 * MeV; //Deprecated - does nothing cs["rfBGElectronSpectrum"] = "Fixed"; //Deprecated - does nothing cs["rfBGPhotonSpectrum"] = "Fixed"; //Deprecated - does nothing cs["rfBGElectronSpectrumFile"] = ""; //Deprecated - does nothing cs["rfBGPhotonSpectrumFile"] = ""; //Deprecated - does nothing cs["rfBGMultipleSpectraFile"] = "None"; //Deprecated - does nothing cs["rfBGBankFile"] = "None"; //Deprecated - does nothing cs["rfBGSamplingMode"] = "Loop"; //Deprecated - does nothing cd["rfBGTimeWindow"] = 0.2 * ns; //Deprecated - does nothing cd["rfBGTimeDelay"] = 0.0 * ns; //Deprecated - does nothing cd["rfBGZstart"] = 0.0 * ns; //Deprecated - does nothing cd["rfBGRadius"] = 150.0 * mm; //Deprecated - does nothing cd["rfBGScaleFactor"] = 1.0; //Deprecated - does nothing // Digitization Application Calorimeter Controls cd["EMCalAttLengthLong"] = 2400.0 * mm; //The EM Calorimeter models the number of photoelectrons entering the PMT using Interface/src/EMCalDigit.cc cd["EMCalAttLengthShort"] = 200.0 * mm; cd["EMCalAttLengthLongNorm"] = 0.655 * mm; cd["EMCalAttLengthShortNorm"] = 0.345 * mm; cd["EMCalLightCollectionEff"] = 0.031; cd["EMCalEnergyPerPhoton"] = 0.125 * keV; cd["EMCalLightSpeed"] = 170.0 * mm / ns; cd["EMCalLightGuideEff"] = 0.85; cd["EMCalQuantumEff"] = 0.18; cd["EMCalAmplificationCof"] =1000000.; cd["EMCalAmplificationFluct"] = 1000.; cd["EMCalAdcConversionFactor"] = 0.25*1e-12*coulomb; // pC per count cd["EMCalTdcConversionFactor"] = 0.025 * ns; ci["EMCalAdcThreshold"] = 2; // adc counts cd["EMCalTdcThreshold"] = 1.84*1e-12*coulomb; // pC cd["EMCalTdcResolution"] = 0.05 * ns; ci["EMCalTdcBits"] = 12; cs["EMCalHardCodedTrigger"] = "False"; cd["EMCalSamplingTimeStart"] = 100.0 * ns; cd["EMCalSamplingTimeWindow"] = 100.0 * ns; cd["EMCalElectronicsDecayTime"] = 8.0 * ns; // Digitization Application SciFi controls cs["SciFiDeadChanFName"] = ""; ci["SciFiMUXNum"] = 7; cd["SciFiFiberDecayConst"] = 2.7; cd["SciFiFiberConvFactor"] = 3047.1; cd["SciFiFiberRefractiveIndex"] = 1.6; cd["SciFiFiberCriticalAngle"] = 0.4782 * rad; cd["SciFiFiberTrappingEff"] = 0.056; cd["SciFiFiberMirrorEff"] = 0.6; cd["SciFiFiberTransmissionEff"] = 0.8; cd["SciFiMUXTransmissionEff"] = 1.0; cd["SciFiFiberRunLength"] = 5000.0 * mm; //ME this number is wrong cd["SciFivlpcQE"] = 0.8; cd["SciFivlpcEnergyRes"] = 4.0 * MeV; cd["SciFivlpcTimeRes"] = 0.2 * ns; ci["SciFiadcBits"] = 8; cd["SciFiadcFactor"] = 6.0; ci["SciFitdcBits"] = 16; cd["SciFitdcFactor"] = 1.0; ci["SciFinElecChanPerPlane"] = 1429; ci["SciFinPlanes"] = 3; ci["SciFinStations"] = 5; ci["SciFinTrackers"] = 2; // Digitization Application TOF controls cd["TOFconversionFactor"] = 10 * keV; cd["TOFpmtTimeResolution"] = 100.0 * picosecond; cd["TOFattenuationLength"] = 140 * cm; cd["TOFadcConversionFactor"] = 0.125; cd["TOFtdcConversionFactor"] = 25.0 * picosecond; cd["TOFpmtQuantumEfficiency"] = 0.25; cd["TOFscintLightSpeed"] = 170.0 * mm / ns; // Digitization Application Ckov controls cd["CKOVadcConversionFactor"] = 0.125; cd["CKOVtdcConversionFactor"] = 25.0 * picosecond; cd["CKOVpmtTimeResolution"] = 100.0 * picosecond; // Reconstruction Application controls cd["BeamCharge"] = 1.0; cd["SciFiTrackRecStatusCut"] = 2.0; cd["SciFiTrackRecRCut"] = 0.0; cd["SciFiTrackRecNHitCut"] = 4.0; cd["SciFiTrackRecNPECut"] = 2.0; cd["SciFiTrackRecChi2Cut"] = 10.0; cd["SciFiTripletChi2Cut"] = 10.0; cd["SciFiadcFactor"] = 6.0; cd["SciFitdcFactor"] = 1.0; cd["SciFiCombineWidth"] = 0.0 * mm; cd["SciFiCombineTime"] = 2.0 * ns; cd["SciFiCombineRadius"] = 1.5 * mm; cd["RecP"] = -1 * MeV; /*ME - new ones*/ cs["DBServerHostName"] = "micewww.pp.rl.ac.uk"; //Database server host name ci["DBServerPort"] = 4443; //Database server port ci["TofTriggerStation"] = 1; // The Station which is giving the trigger ci["RecLevel"] = 5; // 1 = clusters, 2 = points, 3 = tracks, 4 = matching, 5 = pid ci["TofRecLevel"] = 1; // 1 = standard track reconstruction ci["TofCalibrationMode"] = 0; // 0 = reconstruct data, 1 = calculate calibration ci["BeamMakerMode"] = 1; //Matched in tracker/trace ellipse of constant amplitude/uniform distribution... see application for details ci["BeamMakerPID"] = +2; //1=e, 2=mu, 3=pi, 4=K, 5=p, sign=charge (same as ICOOL for003.dat definition) cd["ZStart"] = 0.; //Initial z (absolute) for the BeamMaker application cd["Q7Gradient"] = 1.; //|g0| in T/m for Quadrupole 7 (assumed focussing in x) cd["Q8Gradient"] = 1.; //|g0| in T/m for Quadrupole 8 (assumed defocussing in x) cd["Q9Gradient"] = 1.; //|g0| in T/m for Quadrupole 9 (assumed focussing in x) cd["Q7Current"] = 174.09; //|I| in Amps for Quadrupole 7 (assumed focussing in x, default implies |g0| = 1 T/m) cd["Q8Current"] = 174.09; //|I| in Amps for Quadrupole 8 (assumed defocussing in x, default implies |g0| = 1 T/m) cd["Q9Current"] = 174.09; //|I| in Amps for Quadrupole 9 (assumed focussing in x, default implies |g0| = 1 T/m) cd["Iperg0"] = 174.09; //The current required to get a central gradient of 1 T/m in Quadrupoles 7, 8, and 9 ci["PlotFrequency"] = 100; //For applications which plot histograms to the screen: how many events between updating the plots on the screen? cd["MinimumTOF"] = 0. * ns; //Temporary PID cd["MaximumTOF"] = 100. * ns;//Temporary PID ci["UseRecCuts"] = 0; //If set to 0, do not use the reconstruction cuts defined below. Otherwise assume all events outside cuts are bad. cd["RecMinPX"] = -200 * MeV; //Cut value for reconstructed x momentum cd["RecMaxPX"] = 200 * MeV; //Cut value for reconstructed x momentum cd["RecMinPY"] = -200 * MeV; //Cut value for reconstructed y momentum cd["RecMaxPY"] = 200 * MeV; //Cut value for reconstructed y momentum cd["RecMinPT"] = 0 * MeV; //Cut value for reconstructed transverse momentum cd["RecMaxPT"] = 200 * MeV; //Cut value for reconstructed transverse momentum cd["RecMinPZ"] = 50 * MeV; //Cut value for reconstructed z momentum cd["RecMaxPZ"] = 500 * MeV; //Cut value for reconstructed z momentum ci["WriteDST"] = 0; //Set to 1 to write only TOF data and Zustand vectors after recontruction. Else write everything. ci["NavigatorVerbosity"] = 0; //Set Kalman verbosity level ci["FitterVerbosity"] = 0; //Set Kalman verbosity level ci["SetupVerbosity"] = 0; //Set Kalman verbosity level ci["ModelVerbosity"] = 0; //Set Kalman verbosity level ci["MatchingVerbosity"] = 0; //Set Kalman verbosity level cd["KalmanStepSize"] = 10. * cm; //Step size for Kalman fitter; used if fields are not constant ci["KalmanUseFieldMap"] = 0; //Set to 0 to use a constant field for track fits; set to 1 to use BeamTools (real) fields for reconstruction // Analysis Application controls cs["AnalysisParametersFile"] = "AnaParams.dat"; //Auxiliary file for analysis; see $MICESRC/Analysis/doc/ cs["ICOOLfor003StyleFile"] = "for003.dat"; //icool beam input data file cs["ICOOLfor009StyleFile"] = "for009.dat"; //icool beam output data file ci["AnalysisParticlePdgId"] = -13; //PDG Particle ID; other events will not be used in the analysis ci["StartEvent"] = 0; //Start event - ignores events before this cd["TransferMapAbsoluteError"] = 1e-5; //Absolute error when Optics package calculates transfer maps cd["TransferMapRelativeError"] = 1e-5; //Relative error when Optics package calculates transfer maps cd["OpticsStepSize"] = 100 * mm; //Step size for Optics package cs["OpticsFileName"] = "Optics.out"; //Output file name for Optics package cs["OpticsdEdXModel"] = "BetheBloch"; //dEdx model for optics package; "MinimumIonising" or "BetheBloch" ci["OpticsCalculationOrder"] = 1; //Default order for calculation of optics transfer maps (>1 still doesn't work I'm afraid) cs["PidInputFile"] = "nnReadStage6.root"; //Input PID data file for PIDAnalysis application cs["PidTreeName"] = "eventTree;7"; //Input Tree name for PIDAnalysis application cd["PidBGWeight"] = 1.; // Weighting given to background events in PidAnalysis application ci["PidAnalysisPlanes"] = 1; // Planes used in PidAnalysis application 1 = tracker ref, 2 = tof ref central, 3 = tof ref outer, negative = same with smearing //***End Doc Script*** // Example of use of InputDataCardsVector // double avtest[4] ={1.,2.,3.,4.}; // fillVector("VectorTest",4,avtest); // The equivalent entry in the input file is: // VectorTest 4 1. 2. 3. 4. // An alternative for the case where default values are all zero is // cv["VectorTest"] = vector(4); } dataCards::~dataCards() { } void dataCards::fillVector(const char* st, const int& nentries, const double* entry) { vector cvec(nentries); for(int i=0; i> t; if (t.length() == 0) continue; if (t[0] == '#') continue; // Comments cards ignored if (t[0] == '!') continue; // MCFast style comment int ok = 0; InputDataCardsDouble::iterator i = cd.find(t); if ( i != cd.end()) { double d; is >> d; cd[t] = d; ok = 1; } if( ok == 0) { InputDataCardsInt::iterator i1 = ci.find(t); if(i1 != ci.end()){ int ii; is >> ii; ci[t] = ii; ok =1; } } if (ok == 0) { std::istringstream is2(c); is2 >> t; InputDataCardsString::iterator i2 = cs.find(t); if ( i2 != cs.end()) { std::string s2; is>> s2; cs[t] = s2; ok = 1; } } if (ok == 0) { std::istringstream iv(c); iv >> t; InputDataCards3Vector::iterator i2 = c3v.find(t); if ( i2 != c3v.end()) { Hep3Vector v; iv >> v; c3v[t] = v; ok = 1; } } if (ok == 0) { InputDataCardsVector::iterator i2 = cv.find(t); if ( i2 != cv.end()) { int nentries; is >> nentries; vector cvec(nentries); for(int i=0; i> vd; } else { throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Error reading key "+t+". Bad data format", "dataCards::readKeys")); } cvec[i] = vd; } cv[t] = cvec; ok = 1; } } if (ok != 1) throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Failed to recognise datacard "+t+".", "dataCards::readKeys")); } return 1; } double dataCards::fetchValueDouble(const std::string& key) { InputDataCardsDouble::iterator i=cd.find(key); if (i == cd.end()) throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Error fetching unknown datacard "+key+".", "dataCards::fetchValueDouble")); return i->second; } int dataCards::fetchValueInt(const std::string& key){ InputDataCardsInt::iterator i=ci.find(key); if( i == ci.end()) throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Error fetching unknown datacard "+key+".", "dataCards::fetchValueInt")); else return i->second; InputDataCardsDouble::iterator i2=cd.find(key); // only gets here if not if( i2 == cd.end()) // stored as int throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Error fetching unknown datacard "+key+".", "dataCards::fetchValueInt")); return (int) i->second; } Hep3Vector dataCards::fetchValue3Vector(const std::string& key) { InputDataCards3Vector::iterator i=c3v.find(key); if (i == c3v.end()) throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Error fetching unknown datacard "+key+".", "dataCards::fetchValue3Vector")); return i->second; } std::string dataCards::fetchValueString(const std::string& key) { InputDataCardsString::iterator i=cs.find(key); if (i == cs.end()) throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Error fetching unknown datacard "+key+".", "dataCards::fetchValueString")); return i->second; } std::vector dataCards::fetchValueVector(const std::string& key) { InputDataCardsVector::iterator i=cv.find(key); if (i == cv.end()) throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "Error fetching unknown datacard "+key+".", "dataCards::fetchValueVector")); return i->second; } void dataCards::printValue(const std::string& key) { InputDataCardsDouble::iterator id=cd.find(key); if (id != cd.end()) { std::cout << id->second; return; } InputDataCardsInt::iterator in=ci.find(key); if (in != ci.end()){ std::cout << in->second; return; } InputDataCards3Vector::iterator i3v=c3v.find(key); if (i3v != c3v.end()) { std::cout << i3v->second; return; } InputDataCardsString::iterator is=cs.find(key); if (is != cs.end()) { std::cout << is->second; return; } InputDataCardsVector::iterator iv=cv.find(key); if (iv != cv.end()) { std::vector v = iv->second; for (unsigned int i = 0; i < v.size(); i++) { if (i==0) std::cout << "("; else std::cout << ","; std::cout << v[i]; } std::cout << ")"; return; } throw(MAUS::Exceptions::Exception(MAUS::Exceptions::recoverable, "datacard "+key+" not found.", "dataCards::printValue")); } std::ostream& operator<<(std::ostream& o, const dataCards& d) { o << " ============== DataCards ==============" << endl; InputDataCardsString::const_iterator si = d.cs.begin(); for (; si != d.cs.end(); ++si) { o << " " << si->first << " = " << si->second << endl; } o << " ---------------------------------------" << endl; InputDataCardsInt::const_iterator ii = d.ci.begin(); for (; ii != d.ci.end(); ++ii) { o << " " << ii->first << " = " << ii->second << endl; } o << " ---------------------------------------" << endl; InputDataCardsDouble::const_iterator di = d.cd.begin(); for (; di != d.cd.end(); ++di) { o << " " << di->first << " = " << di->second << endl; } o << " ---------------------------------------" << endl; InputDataCards3Vector::const_iterator v3i = d.c3v.begin(); for (; v3i != d.c3v.end(); ++v3i) { o << " " << v3i->first << " = " << v3i->second << endl; } o << " ---------------------------------------" << endl; InputDataCardsVector::const_iterator vi = d.cv.begin(); for (; vi != d.cv.end(); ++vi) { o << " " << vi->first << " = ("; std::vector v = vi->second; for (unsigned int i = 0; i < v.size(); i++) { if (i>0) o << ","; o << v[i]; } o << ")" << endl; } o << " =======================================" << endl; return o; }