Difference between revisions of "Analysis TTreeFormat"
From GlueXWiki
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"Identifier": (unsigned int)[] //each particle has it's own # | "Identifier": (unsigned int)[] //each particle has it's own # | ||
"ParentIdentifier": (unsigned int)[] //the "Identifier" of the particle this particle decayed from (0 if none (e.g. photoproduced)) | "ParentIdentifier": (unsigned int)[] //the "Identifier" of the particle this particle decayed from (0 if none (e.g. photoproduced)) | ||
− | "PID_PDG": | + | "PID_PDG": int[] |
//KINEMATICS: THROWN //At the production vertex | //KINEMATICS: THROWN //At the production vertex |
Revision as of 11:02, 24 April 2013
Contents
Why a standard TTree format?
- For any reaction can streamline (and provide a best-practices implementation/examples of): analysis utilities, BDT setup/input, amplitude analysis setup/input(?)
- Makes it easy for users to keep everything organized, especially handling of the combinatoric background.
- Output can be enabled/disabled with a single flag.
- Format is designed to be one-size-fits-all, but is still extensible (customizable).
TTree Format - General
ROOT Version
- ROOT >= v5.32 will be required for building BANA
- Much easier to code TTree creation: TClonesArray::ConstructedAt() can be used to replace calls to placement-new
- Just about any version of ROOT is fine for reading the data
Supporting Both TTree::Draw() & Object-Oriented Programming
- Each variable will have it's own TBranch.
- This allows access to TTree::Draw(), etc. for quick, simple access to the data.
- For object-oriented access to the data:
- Will provide tool to convert tree branch data into the C++ objects for a given event (callable from TSelector::Process())
- C++ classes (similar to DANA classes): DTreeEvent, DTreeCombo, DTreeStep, DTreeParticle (compiled into ROOT dictionary & loadable shared library)
- Can be used to write/execute reusable software that will work for any reaction (e.g. handling double-counting when filling histograms)
Reactions, Events, and Branches
- One TTree per DReaction
- e.g., will have different trees for missing/detected recoil proton for the same final state
- One TTree entry per recorded physics event.
- Each variable will have it's own TBranch
- Branch name format: "UniqueParticleName__VariableName" //note double underscore (so that the variable & particle names can have single underscores)
- Positions and four-momenta will be stored in TVector3 & TLorentzVector objects, all others variables are double or unsigned int.
- Users can add their own custom branches to the tree
Particle Combinations
- In a given entry, the TBranch for each variable holds an array: each index of the array corresponds to a different particle combination.
- So all of the data from particle combination #3 will be stored in index "2" of each array
- This excludes data like run#, thrown particles, etc.
- Combos will be sorted in the arrays by kinematic fit FOM (if no kinfit performed, then by overall pid FOM) (best listed first)
- TObject data (e.g. TLorentzVector, TVector3) will be stored in TClonesArray's
Event-Independent Information
- Stored in TTree::fUserInfo (a TList*)
- TMap of "UniqueParticleName" (TObjString) -> Particle_t (actually an unsigned int stored in TObjString)
- Decays:
- TMap of particle decays: "UniqueParticleName" of decaying particles (TObjString) -> "UniqueParticleName" of decay products (TClonesArray(TObjString))
- TMap of decay products: "UniqueParticleName" of decay product (TObjString) -> "UniqueParticleName" of decaying particle (TObjString)
Saved Data
- Event identification: run#, event#, #particle combinations
- All particle data in all particle combinations (kinematics, PID chisq, dE/dx, etc.)
- All detected particle hypotheses that are not used in any of the recorded particle combinations
- All thrown particle data
- Miscellaneous data: kinematic fit chisq, rf time, target type, etc.
TTree Format - Detail
- Example Reaction:
- γ p → η'1(2300), p
- η'1(2300) → K*(892)0, K0_bar
- K*(892)0 → K+, π-
- K0_bar → π+, π-
- K*(892)0 → K+, π-
- η'1(2300) → K*(892)0, K0_bar
- γ p → η'1(2300), p
Unique Particle Names
- Reaction Particle Names, Detected: "Proton," "KPlus," "PiMinus1," "PiPlus," "PiMinus2"
- Reaction Particle Names, Decaying: "EtaPrime1_2300," "KStar892_0," "KShort"
- No branches are created for these particles. All of their properties are derivable from the other data in the tree
- Thrown MC Particle Name: "Thrown"
- Array entries do NOT correspond to particle combos: just a different particle in each array index
- Unused Particle Hypothesis Name: "Unused"
- Array entries do NOT correspond to particle combos: just a different particle in each array index
Particle Data : Detected Reaction Particles
"Identifier": (unsigned int)[] //each physical particle has it's own # (to keep track of different pid hypotheses for the same particle) //KINEMATICS: MEASURED //At the production vertex "Position_Measured": TClonesArray(TVector3) //the production vertex "Time_Measured": double[] //the measured value in TOF/BCAL/FCAL projected back to Position_Measured "P4_Measured": TClonesArray(TLorentzVector) // KINEMATICS: END "Position_End": TClonesArray(TVector3) //the reconstructed position of the BCAL/FCAL/TOF hit "Time_End": double[] "P4_End": TClonesArray(TLorentzVector) //KINEMATICS: KINFIT //At the production vertex //only present if kinfit performed "Position_KinFit": TClonesArray(TVector3) //the production vertex "Time_KinFit": double[] "P4_KinFit": TClonesArray(TLorentzVector) // KINEMATICS: Other "PathLength": double[] //from dPosition_Start to dPosition_End // PID QUALITY: "NDF_Tracking": (unsigned int)[] //for charged only "ChiSq_Tracking": double[] //for charged only "NDF_Timing": (unsigned int)[] "ChiSq_Timing": double[] //using kinematic fit data "ChiSq_Timing_Measured": double[] //using measured data "NDF_DCdEdx": (unsigned int)[] //for charged only "ChiSq_DCdEdx": double[] //for charged only // DEPOSITED ENERGY: "dEdx_CDC": double[] //for charged only "dEdx_FDC": double[] //for charged only "dEdx_TOF": double[] //for charged only "dEdx_ST": double[] //for charged only "Energy_BCAL": double[] "Energy_FCAL": double[]
Particle Data : Unused Hypotheses
"Identifier": (unsigned int)[] //each physical particle has it's own # (to keep track of different pid hypotheses for the same particle) "PID": (unsigned int)[] //Particle_t value //KINEMATICS: MEASURED //At the production vertex "Position_Measured": TClonesArray(TVector3) //the production vertex "Time_Measured": double[] //the measured value in TOF/BCAL/FCAL projected back to Position_Measured "P4_Measured": TClonesArray(TLorentzVector) // KINEMATICS: END "Position_End": TClonesArray(TVector3) //the reconstructed position of the BCAL/FCAL/TOF hit "Time_End": double[] "P4_End": TClonesArray(TLorentzVector) // KINEMATICS: Other "PathLength": double[] //from Position_Measured to Position_End // PID QUALITY: "NDF_Tracking": (unsigned int)[] //for charged only "ChiSq_Tracking": double[] //for charged only "NDF_Timing": (unsigned int)[] "ChiSq_Timing": double[] //using kinematic fit data "ChiSq_Timing_Measured": double[] //using measured data "NDF_DCdEdx": (unsigned int)[] //for charged only "ChiSq_DCdEdx": double[] //for charged only // DEPOSITED ENERGY: "dEdx_CDC": double[] //for charged only "dEdx_FDC": double[] //for charged only "dEdx_TOF": double[] //for charged only "dEdx_ST": double[] //for charged only "Energy_BCAL": double[] "Energy_FCAL": double[]
Particle Data : Thrown
"Identifier": (unsigned int)[] //each particle has it's own # "ParentIdentifier": (unsigned int)[] //the "Identifier" of the particle this particle decayed from (0 if none (e.g. photoproduced)) "PID_PDG": int[] //KINEMATICS: THROWN //At the production vertex "Position_Thrown": TClonesArray(TVector3) //the production vertex "Time_Thrown": double[] "P4_Thrown": TClonesArray(TLorentzVector)
Accessing TClonesArray Data Examples
- TSelector:
GetEntry(entry); cout << ((TLorentzVector*)PiPlus2__Momentum_Measured->At(0))->Px() << endl; //At(): particle combination 0, 1, 2, ...
- TTree:
MyTree->Draw("PiPlus2__Momentum_Start->Px()"); //draws all particle combinations
C++ Classes
- Data Structures:
- DTreeParticle: roughly mirrors DKinematicData: kinematics + PID info of track
- DTreeStep: roughly mirrors DParticleComboStep: collection of DTreeParticle's for a given step of a reaction (e.g. photoproduction, Λ decay, π0 decay, etc.)
- DTreeCombo: roughly mirrors DParticleCombo (collection of DTreeStep's for a given reaction), + detected particles not used in the combo
- DTreeEvent: contains DTreeCombo's for each output DReaction, + thrown tracks
- Extensible:
- Each class has maps to contain additional data (TObject* and double, map keys are string): custom branches in the TTree will be added here.
- Usage:
- Process with a TSelector.
- TTree::Draw() and TTree::Project() will not work due to nested classes/containers.
DTreeParticle
- Roughly mirrors DKinematicData: kinematics + PID info of track
- p3, v3, and t are stored at both the start (production) and end points (decay, TOF/BCAL/FCAL hit) of the track.
- This is primarily motivated by the Ξ-, which is long-lived and whose trajectory is bent by the magnetic field before it decays.
- Extensible: maps can be used by users to add their own custom information.
class DTreeParticle : public TObject { public: // PID: Particle_t dPID; // KINEMATICS: Start //If kinematic fit was performed, this is the kinematic fit results. Else are identical to the "Measured" kinematics. TVector3 dPosition_Start; //the position where the particle is produced double dTime_Start; //time of the track at dPosition_Start TVector3 dMomentum_Start; //momentum of the track at dPosition_Start // KINEMATICS: End TVector3 dPosition_End; //detected particles: the reconstructed position of the BCAL/FCAL/TOF hit; decaying particles: the point where it decays double dTime_End; //time of the track at dPosition_End TVector3 dMomentum_End; //momentum of the track at dPosition_End // KINEMATICS: Measured TVector3 dPosition_Measured; //the position where the particle is produced double dTime_Measured; //time of the track at dPosition_Measured, projected from the TOF/BCAL/FCAL hit TVector3 dMomentum_Measured; //momentum of the track at dPosition_Start // KINEMATICS: Other double dPathLength; //from dPosition_Start to dPosition_End // PID QUALITY: unsigned int dNDF_Tracking; double dChiSq_Tracking; unsigned int dNDF_Timing; double dChiSq_Timing; unsigned int dNDF_DCdEdx; double dChiSq_DCdEdx; // DEPOSITED ENERGY: map<DetectorSystem_t, double> dDepositedEnergies; //Is dE/dx for all but BCAL/FCAL (shower energies) // DTREESTEP POINTERS: const DTreeStep* dProductionStep; //the step object in which this DTreeParticle is produced (is a final-state particle) const DTreeStep* dDecayStep; //the step object in which this DTreeParticle decays (is an initial-state particle) (will be null if not a decaying particle!) // CUSTOM VARIABLES: map<string, double> dCustomVariables; //key is unique string, double is value map<string, const TObject*> dCustomObjects; //key is unique string, TObject* is object ClassDef(DTreeParticle, 1) };
DTreeStep
- Roughly mirrors DParticleComboStep: collection of DTreeParticle's for a given step of a reaction (e.g. photoproduction, Λ decay, π0 decay, etc.)
- Extensible: maps can be used by users to add their own custom information.
class DTreeStep : public TObject { public: // INITIAL PARTICLES: const DTreeParticle* dInitialParticle; //if is null: decaying or beam particle not yet set! const DTreeParticle* dTargetParticle; //NULL for no target // FINAL PARTICLES: deque<DParticle_t> dFinalParticleIDs; //separate in case particle is NULL (e.g. decaying resonance) deque<const DTreeParticle*> dFinalParticles; //particle may be NULL if it is decaying or missing (especially if no kinematic fit was performed!!) // CUSTOM VARIABLES: map<string, double> dCustomVariables; //key is unique string, double is value map<string, const TObject*> dCustomObjects; //key is unique string, TObject* is object ClassDef(DTreeStep, 1) };
DTreeCombo
- Roughly mirrors DParticleCombo (collection of DTreeStep's for a given reaction), + detected particles not used in the combo
- Extensible: maps can be used by users to add their own custom information.
class DTreeCombo : public TObject { public: // STEPS: deque<const DTreeStep*> dTreeSteps; // RF: double dRFTime; // UNUSED PARTICLES: vector<const DTreeParticle*> dUnusedDetectedParticles; vector<const DTreeShower*> dUnusedDetectedShowers; // KINEMATIC FIT: DKinFitType dKinematicFitType; //Defined in DKinFitResults.h //d_NoFit if not performed double dChiSq_KinematicFit; //NaN if not performed unsigned int dNDF_KinematicFit; //0 if not performed // CUSTOM VARIABLES: map<string, double> dCustomVariables; //key is unique string, double is value map<string, const TObject*> dCustomObjects; //key is unique string, TObject* is object ClassDef(DTreeCombo, 1) };
DTreeEvent
- Contains DTreeCombo's for each output DReaction, + thrown tracks
- Extensible: maps can be used by users to add their own custom information.
class DTreeEvent : public TObject { public: // RUN, EVENT #'s: unsigned int dRunNumber; unsigned int dEventNumber; // DATA: map<string, deque<const DTreeCombo*> > dTreeCombos; //string key is (D)Reaction name, deque is the particle combos deque<const DTreeParticle*> dThrownParticles; // CUSTOM VARIABLES: map<string, double> dCustomVariables; //key is unique string, double is value map<string, const TObject*> dCustomObjects; //key is unique string, TObject* is object ClassDef(DTreeEvent, 1) };