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geant4/examples/advanced/composite_calorimeter/README
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-------------------------------------------------------------------
$Id: README,v 1.11 2004/05/18 14:57:48 ribon Exp $
-------------------------------------------------------------------
=========================================================
Geant4 - Composite calorimeter example
=========================================================
README
---------------------
CompositeCalorimeter is an example of a test-beam simulation used
by the CMS Collaboration to validate Geant4 against real data taken
(in 1996) in a CMS Hadron calorimeter test-beam.
The name "Composite" for this example emphasizes that, although the
test-beam had the goal of studying the hadronic calorimeter response,
part of the data was taken with the presence of the electromagnetic
crystal calorimeter in front of the hadronic calorimeter, to better
reproduce the situation as in the real CMS experiment.
The geometry of the simulation has been setup in such a way to allow
very easily, at run time (therefore without need of changing any code;
see below for the details) the inclusion or exclusion of the
electromagnetic calorimeter part.
Although some important aspects, for a detailed comparison between
test-beam data and simulation, like beam profile, noise, and digitization,
have been omitted here (to avoid too many technical details),
nevertheless, this example is able to reproduce the main features of
most of the relevant observables as measured in the real test-beam.
The output of this example, if the AIDA or Anaphe/Lizard environment
has been properly setup (see below), consists of a set of histograms
and one ntuple which are stored on a HBOOK file.
In our opinion, the most original "lesson" which is offered by this
advanced example for the Geant4 user is to show how the Geometry and
the Sensitive/Hit part of the simulation is treated in a big experiment.
Although the details of how this is done vary from experiment to
experiment (it is worth, for instance, to compare with the Atlas-based
advanced example lAr_calorimeter), the main driving needs and goals
are quite general: to have consistency, but avoiding duplications
and couplings as much as possibile, between Simulation, Reconstruction,
and Visualization. Notice that the solution offered in this example
by CMS could appear "overdone" for the sake of simulating only a
relatively simple test-beam setup; but it should be kept in mind
that the same approach is used also for the full CMS detector
simulation, as well as for any subdetector.
1. Setting up the environment variables
---------------------------------------
The user should first setup, as "usual", the Geant4 environmental
variables (in particular, the variable G4ANALYSIS_USE must be set
if you want to have the histograms and the ntuple).
Then the specific setup for this example, including the AIDA/PI part
used in the analysis, should be run:
> source envExample.csh in the case of C-shell
or
> . envExample.sh in the case of bash-shell
The analysis part is based on AIDA/PI.
Please take a look to the web page: http://www.cern.ch/PI .
2. Sample run
-------------
Once the environmental variables are setup, you can get the executable
$G4WORKDIR/bin/$G4SYSTEM/CompositeCalorimeter
by typing "gmake" on this directory.
Then, you can execute it using the Geant4 macro command input file test.g4mac
as follows:
> $G4WORKDIR/bin/$G4SYSTEM/CompositeCalorimeter test.g4mac
which simulate 10 events, each being a 100 GeV pi- incident on the
electromagnetic crystal calorimeter followed by the hadronic calorimeter,
without magnetic field.
The output is the HBOOK file "ccal.his" , which can be seen either with
Lizard (or any other AIDA-compliant package) or with Paw or Root.
See part "8. Analysis / Histogramming" below for more details on the
content of that file.
If you run instead:
> $G4WORKDIR/bin/$G4SYSTEM/CompositeCalorimeter
after having setup the Geant4 visualization variables and the PATH,
you can visualize the geometry of the apparatus, and also see some
events. Similarly, you can get a very simple graphical user interface
that allows to select the particle type, its energy, and the number
of events (between a limited number of possibilities).
For more details, see part "9. Visualization / GUI".
3. Detector description
-----------------------
Let's start with a brief description of the test-beam setup.
There are two possible configurations:
i) HCAL only, that is only the hadronic calorimeter is present;
ii) ECAL+HCAL, that is the electromagnetic calorimeter (ECAL)
is placed in front of the hadronic calorimeter.
ECAL is made of 23 cm long PbWO4 crystals (corresponding to about
25.8 radiation lengths, and 1.1 interaction lengths); for the
test beam a 7 x 7 = 49 matrix of crystals is used.
HCAL is a sampling calorimeter, with plastic scintillator as sensitive
part and copper as absorber. 28 scintillator plates were used with
absorber of varying thickness in between, and also varying thickness
and type of scintillator. More precisely:
--- layer 1: 2 cm of Copper
--- layer 2 to 7: 4 cm of Copper
--- layer 8 to 21: 6 cm of Copper
--- layer 22 to 27: 8 cm of Copper
For the scintillators: 2 mm passive Plastic; 4 mm active Plastic;
1 mm passive Plastic.
The total length of HCAL consists of 152 cm of Copper plus 189 mm of Plastic.
The dimension orthogonal to the beam direction is 64 cm x 64 cm.
The ECAL and HCAL considered here are prototypes for the Central and
Endcap calorimeters of the CMS detector (which covers the rapidity
region |eta| < 3.0 ; CMS has also a Forward calorimeter, which covers
the region 3.0 < |eta| < 5.0, but this part was not considered in
this test-beam setup). Notice, however, that there are more layers
(28 instead of 19 in the Barrel or 18 in the Endcap) of HCAL in the
test-beam setup than in the real CMS detector, in order to study
energy containment. Therefore, the ECAL+HCAL in the test-beam amounts
to more than 11 radiation lengths as for the real CMS detector (the
19 layers of the Barrel have each 6 cm of absorber, whereas the
18 layers of the Endcap have each 6.6 cm of absorber, so that the
number of interaction lengths are rougly the same).
Five values of the magnetic field (parallel to the face of the scintillators)
have been considered in the test-beam: 0.0 , 0.375 , 0.75 , 1.50 , 3.0 Tesla.
In order to set the magnetic field, you have to edit the file
dataglobal/fmap.tb96
and change the first number (which appears in the third line of
that file, on the first column; the unit being Tesla):
#. Field map
*DO FLDM
0.0 9 652.0
for example, if you want a magnetic field of 3.0 Tesla the last
line must be set as follows (the magnetic field unity is kilo Gauss).
30.0 9 652.0
The default stepper in magnetic field is G4ClassicalRK4, but other
possibilities can be selected by editing the file
src/CCalDetectorConstruction.cc (look at the string "***STEPPER***").
In order to deactivate either the ECAL or the HCAL, it is enough
to comment out the corresponding line in the file g4testbeamhcal96.conf,
using "#" as the comment character. For instance, to have only the HCAL
without ECAL:
"HcalTB96" "tbhcal96" 1
#"CrystalMatrixModule" "tbhcal96xtal" 1
In this test-beam setup, at the back of ECAL, there is also some
material for support and readout, which has been considered in the
simulation. For the HCAL, only the fibres are close to the test-beam,
and because they have the same composition as the scintillators
they are adequately represented in the simulation; the remaining
of the readout, including the photomultipliers, are in readout boxes
far away from the HCAL, and hence are not present in the simulation.
Let's summarizes now the geometry description of the simulation.
As said in the introduction, this part is the most original and
important of this example, but it is quite complex and can be fully
appreciated only in the context of the CMS software framework, in
particular in the relation between Simulation, Reconstruction, and
Visualization. Therefore we limit ourself to only few considerations,
pointing to the internal CMS documentation for more details.
--- In order to share the same geometrical and physical information
about CMS between Simulation, Reconstruction, and Visualization,
avoiding inconsistencies, duplications, and unnecessary dependecies,
all these information is store, once for all, in common databases
(typically in XML format), instead of putting them inside C++ classes,
as usually done in simpler detector descriptions (in most of the
the Geant4 examples, novice or advanced, the geometry information
is kept inside the concrete class which inherits from
G4VUserDetectorConstruction). For simplicity, in this example,
these "databases" are nothing more than ASCII files:
datageom/ : tbhcal96.geom, tbhcal96hcal.geom, tbhcal96xtal.geom
store the information about the experimental Hall,
the HCAL, and the ECAL, respectively.
dataconf/ : g4testbeamhcal96.conf, testbeamhcal96.conf
store the information about which configuration
(HCAL only, or ECAL+HACL) is considered, in the
Simulation and Reconstruction, respectively.
dataglobal/ : fmap.tb96, material.cms, rotation.cms
The first one is the magnetic field map (how the
intensity of the magnetic field, in the direction
orthogonal to the beam direction, varies along
the beam axis). The second one, material.cms,
keeps the full collection of all materials used in
the CMS detector (not only in the calorimeters,
although we are simulating only them in this example!).
The third one, rotation.cms, collects a set of useful
rotation parameters (angles).
datavis/ : tbhcal96.vis, tbhcal96hcal.vis, tbhcal96xtal.vis
visualization information for, respectively, the
experimental Hall, HCAL, and ECAL.
--- In order to allow an high degree of flexibility, at the geometry
level the user can choose which subsystem of the detector setup
should be simulated and can activate or deactivate the sensitive
parts, subsystem by subsystem. This can be done at run time,
by modifying one of the above database information, without need
of putting the hands on the code, recompiling, etc.
--- There are two "parallel geometry factories": one described by "core"
classes, which are independent from the Simulation (and therefore
can be used, for instance, by the Reconstruction); and one which
is specific of the Simulation. In the latter case (Geant4 side of
the geometry model), all the geometry factories are derived from the
base class CCalG4Albe. Furthermore, using double inheritance, each
of them derives also from the counterpart in the "core" hierarchy.
The design of the CCalG4Able class helps a modular approach and easy
interchanging at the level of subdetectors, allowing a straightforward
transition from the simulation of the entire CMS detector to that of
just a part of it, or to a test-beam geometry, as indeed in this example.
Of course this modular, flexible, and general approach does not come
for free: the price to pay here is its complexity, which would be
otherwise unjustified if we limited ourself to the pure simulation
of a relatively simple test-beam setup.
--- See "10. Classes Overview" below for a schematic summary of the
various classes involved in the Geometry description of this example.
4. Physics processes
--------------------
By the default, one of the ufficial High Energy Physics List for
Calorimetry, QGSC, is used in this example. However, it is
very easy to use instead either LHEP or QGSP. To do so, it is
enough to comment/uncomment a line in the main CompositeCalorimeter.cc :
for example, if you want to use LHEP instead of the default QGSC
you have to change it as follows:
//***LOOKHERE*** CHOOSE THE PHYSICS LIST.
runManager->SetUserInitialization(new LHEP); // LHEP
// runManager->SetUserInitialization(new QGSP); // QGSP
// runManager->SetUserInitialization(new QGSC); // QGSC
//***endLOOKHERE***
Notice that, for most of the cases (and certainly also in this case
in which we don't even take into account the beam profile, noise
and digitization!) the faster LHEP Physics List would be good enough
for calorimetry studies. However, we prefer to use, as default, the
more sophisticated (but slower) QGSC Physics List for the learning
purposes of this example.
Please refer to the Web page:
http://cmsdoc.cern.ch/~hpw/GHAD/HomePage/index.html
for more information on these (and others) Physics Lists.
Please notice that, for the time being, some classes, which can be
downloaded from the above Web page, have to be included in the
include/ and src/ subdirectories of this example. However, hopefully
soon, these classes will be distributed with Geant4 and therefore their
explicit inclusion in the example will no longer be necessary.
5. Particle Generator
---------------------
The 1996 test-beam has been taken with the following particles:
--- 225 GeV muons (for calibration)
--- 10 to 300 GeV pions
--- 10 to 300 GeV electrons
therefore the standard Geant4 Particle Gun has been used as primary
generator. Notice that, for the sake of keeping the example not too
complicated, the proper simulation of the beam profile and
beam contamination have been neglected.
6. Hits
-------
In CMS there are two groups of hits: Tracker-like and Calorimeter-like.
Only the latter one appears in this example.
For the same reasons, as seen for the Geometry, of consistency without
duplication of information and unnecessary coupling between Simulation,
Reconstruction, and Visualization, the simulation calorimeter hit class,
CCalG4Hit, doubly inherits from the common Geant4 abstract class for
all hits, G4VHit, and from the "core" (i.e. simulation independent)
CMS calorimeter hit class, CCalHit.
A new Hit object is created
- for each new particle entering the calorimeter;
- for each detector unit (i.e cristal or fiber or scintillator layer);
- for each nanosecond of the shower development;
The information stored in each CCalHit object is the following:
- Entry : local coordinates of the entrance point of the particle
in the unit where the shower starts;
- the TrackID : Identification number of the incident particle;
- the IncidentEnergy : kinetic energy of that incident particle;
- the UnitID : the identification number of the detector unit
(crystal, or fiber, or scintillator layer);
- the TimeSlice : the time interval, in nanoseconds, in which the
hit has been created;
- the EnergyDeposit : the energy deposit in this hit.
Notice that all hit objects created for a given shower have the same
values for the first three pieces of information.
No Noise and Digitization
--------------------------
In order to keep the complexity of this example to a reasonable
level, both noise and digitization effects have not been included.
7. User Actions
----------------
In this example. there have been used the following User Actions:
--- G4UserRunAction (the derived, concrete class is CCalRunAction):
it is used to invoke the Analysis object at the beginning of
the Run, to instantiate it and passing it the Run number, and
at the end of the Run, to inform it that the Run is finished
and therefore the histograms, ntuples, etc. must be closed.
--- G4UserEventAction (the derived, concrete class is CCalEndOfEventAction):
it is used to examine, at the end of the Event, all collected
(calorimeter) hits, extract the various observables which are
interesting (to the goal of understanding things like: the effect
of magnetic field on scintiallator; choice of the absorber
thickness by optimizing resolution versus containment; impact of
the absorber depth in the energy caontainment; electromagnetic
calorimeter contribution in the electron - pion separation; etc.)
and finally call the analysis object to store such selected
information on histograms and/or in the ntuple.
The name of the class "CCalEndOfEventAction" is motivated by the
fact that at the beginning of the Event nothing is done.
--- G4UserSteppingAction (the derived, concrete class is CCalSteppingAction):
it is used to extract some "unphysical" information (that is not
experimentally measurable, although interesting for a better
understanding of the shower development), namely the lateral profile
and the deposit as a function of the time (see "8.Analysis/Histogramming
for more details"), which is available only from simulation, and then,
at the end of Event, the analysis object is invoked to store such
information on histograms.
Please notice that the stepping action is not used to create hits.
--- G4UserStackingAction (the derived, concrete class is CCalStackingAction):
it is used to ensure that the same track ID of the particle
originating a shower appears in all hits (calorimeter hit objects
of class CCalHit) of the shower, in any calorimeter part.
8. Analysis / Histogramming
----------------------------
The analysis part of CompositeCalorimeter is kept in class CCalAnalysis,
and is based on the AIDA interfaces and their implementation in PI.
Please take a look to the web page: http://www.cern.ch/PI .
Both the histograms and the ntuple are saved at the end of the run in the
HBOOK file "ccal.his". You can than analyze offline the contents of such
a file, using Lizard (or any other AIDA-compliant package) or with
Paw or Root. Please note that in a multiple run session, the last run
always override the HBOOK file.
What the histograms and the variables of the ntuple represent is
explained below:
Histograms 100 - 127 : energy deposit (in GeV) in the sensitive part
(plastic scintillator layer) of one Hadronic
calorimeter module (there are 28 modules, numbered
from 0 to 27, and the corresponding histogram has
ID = 100 + number of module).
Ntuple variables hcal0 - hcal27 : provide the same information.
Histograms 200 - 248 : energy deposit (in GeV) in one crystal
electromagnetic towers (there are a matrix of
7 x 7 = 49 towers, numbered from 0 to 48, and
the corresponding histogram has
ID = 200 + number of tower).
Ntuple variables ecal0 - ecal48 : provide the same information.
Histograms 300 - 339 : total energy deposit (in GeV) in any
electromagnetic crystal tower or hadronic module
(either in a sensitive or insensitive layer)
in one of the 40 nanosecond time slices: in other
words, histogram 300+I , where I = 0 - 39,
contains the total deposit energy between
I and I+1 nanoseconds after the "collision".
(Notice that the time window considered,
40 nanoseconds, is larger than the LHC
bunch-crossing of 25 nanoseconds.)
Histograms 400 - 469 : energy profile (in GeV), summed over all layers
sensitive (plastic scintillator) and insensitive
(copper absorber), as a function of the radial
distance (in centimeter) from the beam axis
( ID histo = 400 + radial distance in cm ).
Histogram 4000 : total energy deposit (in GeV) in the sensitive parts
of either the electromagnetic or hadronic calorimeters.
Ntuple variable edep provides the same information.
Other ntuple variables are the following:
--- elab : energy (in GeV) of the incident particle.
--- xpos, ypos, zpos : position (in mm) from where the projectile
has been shot.
--- edec, edhc : total energy deposit (in GeV) in the sensitive
parts of, respectively, the electromagnetic
and hadronic calorimeters. Notice that their
sum edec+edhc coincides with edep
Notice that lateral profile (400-469) and time-slice (300-339)
histograms show purely Monte Carlo quantities, which cannot be
experimentally measured.
Please be careful that the range of the histograms has been chosen
in such a way to contain most of the entries, but only few histograms
fill a large fraction of that range, whereas the remaining majority
fill only the first few bins (corresponding to lower energy), and,
therefore, when plotted they look almost empty, but they are not,
and the results are sensible. We suggest to plot the ntuple's variables,
rather than the histograms, when the same information is available
from the ntuple.
9. Visualization / GUI
-----------------------
If you setup one of the following Geant4 environmental variables:
G4VIS_USE_DAWN
G4VIS_USE_VRML
G4VIS_USE_OPENGLX
which correspond to the use of DAWN, VRML, and OPENGLX, respectively,
as visualization engine of Geant4, and set properly the corresponding
PATH as well, it is then possible to visualize the detector and also
some events.
To do so, you have to run
> $G4WORKDIR/bin/$G4SYSTEM/CompositeCalorimeter
without input file: you then see the detector; after that,
you can select the particle gun and its energy, in the
case you want something different from the the default
(which is a 100 GeV pi-), for example:
Idle> /gun/particle e-
Idle> /gun/energy 200 GeV
and then run some events, for example:
Idle> /run/beamOn 3
Notice that, by default, OGLIX is used for the visualization,
because it is quite fast and it does not produce any files in
output. However, you can always choose something else, for example
VRML2FILE or DAWNFILE, either interactively as follows:
Idle> /vis/open DAWNFILE
or by changing the default, by editing the file (main program)
CompositeCalorimeter.cc and comment/uncomment the lines
in such a way to have, at the end:
visCommand = "/vis/open DAWNFILE";
// visCommand = "/vis/open VRML2FILE";
// visCommand = "/vis/open OGLIX";
The tracks that are shown include both charged and neutral particles
of any momentum: if you want instead only charged, or only neutral,
then you have simply to edit src/CCalEndOfEventAction.cc
at the end of the method EndOfEventAction and uncomment the line
where the condition on the charge is made (it should then be
straighforward to eventual add some other conditions, for example
if you want to see only those particles that satisfy certain
kinematic conditions).
Rather than to specify "by hand" the type of particle gun,
its energy, and the number of events, it is possible to have
a very simple GUI (graphical user interface) from which to make
such choices, between a limited set of possibilities, via menus.
Such GUI is based on Motif XmCommand widget, but it would be
straightforward, eventually, to make the necessary changes
in order to use a different one.
The only thing you need to do to get the GUI is to setup
the following Geant4 environmental variables:
G4UI_BUILD_XM_SESSION=1
G4UI_USE_XM=1
Then, if you run the executable without specifying a macro file
(like test.g4mac):
> $G4WORKDIR/bin/$G4SYSTEM/CompositeCalorimeter
a window automatically pops out, with the menus where you
can make your selection of particle type, energy, and number
of events to be run.
10. Classes Overview
---------------------
This is a schematic overview of the classes defined in this example:
CCalPrimaryGeneratorAction
CCalPrimaryGeneratorMessenger
User action for primaries generator.
CCalDetectorConstruction
CCalAMaterial
CCalDataSet
CCalDetector
CCalEcal
CCalEcalOrganization
CCalG4Able
CCalG4Ecal
CCalG4Hall
CCalG4Hcal
CCalGeometryConfiguration
CCalHall
CCalHcal
CCalHcalOrganization
CCalMagneticField
CCalMaterial
CCalMaterialFactory
CCalRotationMatrixFactory
CCalVOrganization
CCalVisManager
CCalVisualisable
CCaloOrganization
CCalutils
Geometry and material definitions for the detector.
Notice in particular that:
CCalHall, CCalEcal, CCalHcal derive from CCalDetector;
CCalG4Hall, CCalG4Ecal, CCalG4Hcal derive from the above
corresponding classes and from CCalG4Able;
CCalEcalOrganization, CCalHcalOrganization derive from
CCalVOrganization : each sensitive cell has an unique
number for detector organization (this is a software
ID not an hardware/electronic one).
CCalHit
CCalG4Hit
CCalG4HitCollection
CCalSDList
CCalSensAssign
CCalSensitiveConfiguration
CCalSensitiveDetectors
CCaloSD
Hit and Sensitive Detectors.
Notice in particular that:
CCalG4Hit derives from G4VHit and CCalHit;
CCaloSD derives from G4VSensitiveDetector.
CCalAnalysis
Analysis manager class which uses Anaphe.
CCalRunAction
User run action class.
CCalEndOfEventAction
User event action class.
CCalStackingAction
User Stacking action class.
CCalSteppingAction
User Stepping action class.
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