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      =========================================================
      Geant4 - an Object-Oriented Toolkit for Simulation in HEP
      =========================================================
 
                             Example Par02
                             -------------
 
  This example is a simplified version of a Geant4-based fast simulation
  program written by Anna Zaborowska for Future Circular Collider (FCC)
  studies.
 
  This example shows how to do "track and energy smearing" in Geant4,
  in order to have a very fast simulation based on assumed detector
  resolutions.
 
  The geometry which is considered is a simplified collider detector set-up,
  inspired by ALEPH/ATLAS/CMS detectors. Although it is much simpler than
  a realistic detector, it is anyhow fairly complex and therefore build up
  from a GDML file, Par02FullDetector.gdml .
 
  In this example:
  -  Particles with transverse momentum less than 1 MeV or pseudorapidity
     larger (in module) than 5.5 are neglected (i.e. the corresponding
     Geant4 track is killed as soon as it is created).
  -  Any primary charged particle is smeared in the tracker as follows:
     its momentum is smeared according to a gaussian, with mean equal to 1.0
     and sigma taken from the momentum resolution of the CMS tracker 
     (with ALEPH or ATLAS tracker as a possible alternative), and then placed
     at the end of the tracker, at the position that it would reach if
     normally transported (i.e. without smearing).
  -  Any primary electron, or positron, or gamma is smeared in the 
     electromagnetic calorimeter as follows: it is killed at the entrance
     of the electromagnetic calorimeter, with a deposited energy equal to
     the gaussian smearing (with mean equal to 1.0 and sigma taken from the
     energy resolution of the CMS electromagnetic calorimeter - with ALEPH or
     ATLAS electromagnetic calorimeter as a possible alternative) of its
     kinetic energy (at the entrance of the electromagnetic calorimeter).
  -  Any primary hadron is smeared in the hadronic calorimeter as follows:
     it is killed at the entrance of the hadronic calorimeter, with a
     deposited energy equal to the gaussian smearing (with mean equal to 1.0
     and sigma taken from the energy resolution of the CMS hadronic 
     calorimeter - with ALEPH or ATLAS hadronic calorimeter as a possible
     alternative) of its kinetic energy (at the entrance of the hadronic
     calorimeter).
  -  The only competing physical processes with respect to the above physics
     parametrisations are the decays.
     Note: no electromagnetic processes;
           no momentum smearing in the tracker for secondary particles; 
           secondary electrons, positrons, gammas in the electromagnetic 
           calorimeter are killed (at the entrance) but without any
           energy deposition; 
           secondary hadrons in the hadronic calorimeter are killed (at the
           entrance) but without any energy deposition.
 
 
  Below some details.
 
 
  1. Detector description
  -----------------------
 
  The geometry is read in from a GDML file, Par02FullDetector.gdml .
 
  The geometry is a simplified collider detector set-up used for the
  first FCC studies, inspired by ALEPH/ATLAS/CMS detectors.
  It is made of 4 main parts: 
  - Tracker
  - Electromagnetic calorimeter
  - Hadronic calorimeter
  - Muon subdetector
 
  In this example, fast simulation parametrisation models exist for the
  first three subdetectors, but not for the Muon subdetector.
  The three parametrisation models:
  - Par02FastSimModelTracker : in the tracker
  - Par02FastSimModelEMCal   : in the electromagnetic calorimeter
  - Par02FastSimModelHCal    : in the hadronic calorimeter
  are build and bound to the respective subdetector (i.e. Geant4 regions)
  in the method: Par02DetectorConstruction::Construct() .
 
  Three configurations are possible for those parametrisation models:
  CMS-like, ALEPH-like, ATLAS-like. 
  By default, the CMS configuration is used.
 
 
  2. Primary generation
  ---------------------
  
  In this example we use a very simple primary generation action,
  Par02PrimaryGeneratorAction, that uses the G4ParticleGun.
  One single particle type, with a well defined energy, and in one fixed
  direction is used for each run: the corresponding values can be set via
  macro commands. See examplePar02.in as an example.
 
  For the FCC studies, Pythia8 events in HepMC format were used for the
  generation of the primary particles.
 
 
  3. Physics List
  ---------------
 
  A special, ad-hoc physics list is used in this example, in order to have
  an ultra-fast parametrised simulation: for all particles, the only two
  physics processes that are assigned are the decay process and the fast
  simulation process. 
  The following three fast simulation models are defined:
 
  - Par02FastSimModelTracker : 
    - bound to the tracker
      (see the method Par02DetectorConstruction::Construct )
    - applicable to all charged particles
      (see the method Par02FastSimModelTracker::IsApplicable )
    - triggered in all cases (i.e. no kinematic constraints)
      (see the method Par02FastSimModelTracker::ModelTrigger )
    - does the following: place the particle at the tracking detector exit 
      (at the place the particle would reach without smearing), and, only
      if the particle is a primary, it smears the momentum of the particle
      according to a gaussian, with mean equal to 1.0 and sigma taken from
      the momentum resolution of the CMS tracker (with ALEPH or ATLAS tracker
      as a possible alternative)
      (see the method Par02FastSimModelTracker::DoIt )
 
  - Par02FastSimModelEMCal : 
    - bound to the electromagnetic calorimeter
      (see the method Par02DetectorConstruction::Construct )
    - applicable to electrons, positrons, gammas
      (see the method Par02FastSimModelEMCal::IsApplicable )
    - triggered in all cases (i.e. no kinematic constraints)
      (see the method Par02FastSimModelEMCal::ModelTrigger )
    - does the following: kill the particle at the entrance of the
      electromagnetic calorimeter, and, only if the particle is a primary,
      it deposits in the electromagnetic calorimeter an energy obtained
      by a gaussian smearing (with mean equal to 1.0 and sigma taken from the
      energy resolution of the CMS electromagnetic calorimeter - with ALEPH
      or ATLAS electromagnetic calorimeter as a possible alternative) of the
      particle kinetic energy (at the entrance of the electromagnetic
      calorimeter)
      (see the method Par02FastSimModelEMCal::DoIt )
 
  - Par02FastSimModelHCal : 
    - bound to the hadronic calorimeter
      (see the method Par02DetectorConstruction::Construct )
    - applicable to all hadrons (i.e. particles made of quarks)
      (see the method Par02FastSimModelHCal::IsApplicable )
    - triggered in all cases (i.e. no kinematic constraints)
      (see the method Par02FastSimModelHCal::ModelTrigger )
    - does the following: kill the particle at the entrance of the
      hadronic calorimeter, and, only if the particle is a primary,
      it deposits in the hadronic calorimeter an energy obtained by a
      gaussian smearing (with mean equal to 1.0 and sigma taken from the
      energy resolution of the CMS hadronic calorimeter - with ALEPH
      or ATLAS hadronic calorimeter as a possible alternative) of the
      particle kinetic energy (at the entrance of the hadronic
      calorimeter)
      (see the method Par02FastSimModelHCal::DoIt )
 
 
  4. User actions, user information and user utility classes 
  ----------------------------------------------------------
 
  - Par02RunAction : run action used for initialization and termination
                     of the run.
 
  - Par02EventAction : event action used for initialization and termination
                       of the event.
 
  - Par02TrackingAction : tracking action used for killing particles with
                          transverse momentum less than 1 MeV or 
                          pseudorapidity larger (in module) than 5.5
                          (see method Par02TrackingAction::PreUserTrackingAction )
                          and to store the information about the track at
                          the end of the simulation of such a track
                          (see method Par02TrackingAction::PostUserTrackingAction ).
 
  - Par02ActionInitialization : initialization of the primary generator class
                                and all user-defined actions (i.e. the three
                                classes above).
 
  - Par02PrimaryParticleInformation : utility class to store information 
                                      associated with a primary particle.
 
  - Par02EventInformation : utility class to store information associated
                            with a Geant4 event.
 
  - Par02DetectorParametrisation : a simple class used to provide the detector
                                   resolution and efficiency, according to the
                                   type of detector: tracker, electromagnetic
                                   calorimeter, hadronic calorimeter.
                                   There are 3 choices: CMS-like (default),
                                   ALEPH-like and ATLAS-like.
                                   The efficiency is currently set to 1.0 in 
                                   all cases and not used.
 
  - Par02Smearer : a simple class that does the gaussian smearing, either
                   of the momentum (in the tracker detector) or in energy
                   (in the electromagnetic or hadronic calorimeter).
 
 
  5. Output
  ---------
 
  The execution of the program (examplePar02) produces in output, at the end
  of a run, a Root file, by default named DefaultOutput.root, which contains
  3 histograms and one ntuple.
 
  The macro file  examplePar02.in  specifies one run made of 1000 events
  each consisting of one 50 GeV electron.
  By editing the file, one could select alternatively a run made of 1000
  events each consisting of one 100 GeV muon, or a run made of 1000 events
  each consisting of one 20 GeV pion- .
 
  See the class Par02Output for the definition of the 3 histograms and the
  ntuples. Here is a quick summary:
  - histogram of the ratio of the momentum smeared and the original momentum
    in the tracker (for primary charged particles);
  - histogram of the ratio of the smeared energy deposited and the original
    energy at the entrance in the electromagnetic calorimeter (for primary
    electrons, positrons and gammas);
  - histogram of the ratio of the smeared energy deposited and the original
    energy at the entrance in the hadronic calorimeter (for primary hadrons);
  - ntuple containing the "Monte-Carlo true" information regarding the
    primary, and the resolution, efficiency, smeared momentum (tracker),
    smeared energy (calorimeter) and impact position (calorimeter) of each
    subdetector (tracker, electromagnetic calorimeter, hadronic calorimeter)
    where the primary is parametrised (tracker and electromagnetic calorimeter
    in the case of primary electrons, positrons and gammas; tracker and
    hadronic calorimeter in the case of primary hadrons; tracker only for
    all other primary charged particles, e.g. muons).
 
  Note:
  - you do not need to have the Root package available to run this example,
    but you need it if you want to look at the histograms and the ntuple
    contained in the Root output file;
  - sensitive detectors and hits are not used in this example.
 
 
  6. How to build and run the example
  -----------------------------------
 
 - You need to have built the Geant4 persistency/gdml module by having set
   the  -DGEANT4_USE_GDML=ON  flag during the CMAKE configuration step, 
   as well as the  -DXERCESC_ROOT_DIR=<path_to_xercesc>  flag pointing to 
   the path where the XercesC XML parser package is installed in your system.
  
 - Compile and link to generate the executable (in your CMAKE build directory):
   %  make
 
 - Execute the application:
   %  examplePar02  examplePar02.in
 
   which produces one Root file: DefaultOutput.root .
 

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