]>
Commit | Line | Data |
---|---|---|
50837721 | 1 | /************************************************************************** |
2 | * Copyright(c) 1998-1999, ALICE Experiment at CERN, All rights reserved. * | |
3 | * * | |
4 | * Author: The ALICE Off-line Project. * | |
5 | * Contributors are mentioned in the code where appropriate. * | |
6 | * * | |
7 | * Permission to use, copy, modify and distribute this software and its * | |
8 | * documentation strictly for non-commercial purposes is hereby granted * | |
9 | * without fee, provided that the above copyright notice appears in all * | |
10 | * copies and that both the copyright notice and this permission notice * | |
11 | * appear in the supporting documentation. The authors make no claims * | |
12 | * about the suitability of this software for any purpose. It is * | |
13 | * provided "as is" without express or implied warranty. * | |
14 | **************************************************************************/ | |
15 | ||
16 | /* $Id$ */ | |
17 | ||
88cb7938 | 18 | ========================================================== |
19 | Please add to this README file all information concerning | |
20 | config files, simulation, digitalization, clusterization, | |
21 | reconstruction and macro analysis | |
22 | ||
6b1e4b22 | 23 | ========================================================== |
24 | How to check that your aliroot is working well | |
25 | ========================================================== | |
26 | There is a script file AlirootRun_MUONtest.script which | |
27 | allows for simulating, reconstructing and making the | |
28 | invariant analysis of the generated Upsilon (1S). | |
29 | The used configuration file is Config.C in MUON | |
30 | directory. | |
31 | There you have to type : | |
32 | ||
33 | source $ALICE_ROOT/MUON/AlirootRun_MUONtest.script | |
34 | ||
35 | If you do not recover a few Upsilons in their mass region | |
36 | in the file MUONmassPlot.root | |
37 | ||
88cb7938 | 38 | ========================================================== |
7985603c | 39 | How to run a MUON generation |
88cb7938 | 40 | ========================================================== |
41 | aliroot | |
fc1fafa5 | 42 | root [0] gAlice->Run(10,"$ALICE_ROOT/MUON/Config.C"); |
88cb7938 | 43 | |
44 | 1 single muon of 7 GeV/c in the MUON spectrometer | |
45 | acceptance will be simulated using geant3. | |
46 | Hit information will be store in the root file in the | |
47 | execution directory. | |
88cb7938 | 48 | If you want to change the option or to define a new directory |
49 | for hits, you have to do the following before: | |
50 | root [0] gAlice->SetConfigFunction("Config( \"/home/martinez/aliroot/work_NewIO/test/\" , \"box\" );"); | |
51 | ||
88cb7938 | 52 | ============================================================ |
53 | How to run MUONCheck macro | |
54 | ============================================================ | |
55 | To check the content of a root data file, the MUONCheck | |
56 | provides a ascii output on screen. | |
57 | ||
58 | To compile MUONCheck.C | |
2058bf30 | 59 | .includepath $ALICE_ROOT/STEER |
60 | .includepath $ALICE_ROOT/MUON | |
bf485fb9 | 61 | .includepath $ALICE_ROOT/MUON/mapping |
2058bf30 | 62 | .L $ALICE_ROOT/MUON/MUONCheck.C++ |
bf17dbfd | 63 | To Load |
64 | gSystem->Load("$ALICE_ROOT/MUON/MUONCheck_C.so") | |
2058bf30 | 65 | |
278a86d5 | 66 | To print Kine : (default file is galice.root ) |
2b32c661 | 67 | MUONkine() or MUONkine("galice.root",##) for the event number ## |
88cb7938 | 68 | |
69 | To print hits : (default file is galice.root if not MUONhits("toto.root""); ) | |
2b32c661 | 70 | MUONhits() or MUONhits("galice.root",##) for the event number ## |
88cb7938 | 71 | |
72 | To print digits : (default file is galice.root) | |
2b32c661 | 73 | MUONdigits() or MUONdigits("galice.root",##) for the event number ## |
88cb7938 | 74 | |
75 | To print rawcluster : (default file is galice.root) | |
2b32c661 | 76 | MUONrecpoints() or MUONrecpoints("galice.root",##) for the event number ## |
88cb7938 | 77 | |
78 | To print trigger : (default file is galice.root) | |
82a59e4b | 79 | MUONrectrigger() or MUONrectrigger("galice.root",##) for the event number ## |
2b32c661 | 80 | |
81 | .... | |
88cb7938 | 82 | |
02d8f072 | 83 | ============================================================ |
6570c14d | 84 | How to check the Geometry |
02d8f072 | 85 | ============================================================ |
fc1fafa5 | 86 | gAlice->Init("$ALICE_ROOT/MUON/Config.C"); |
02d8f072 | 87 | .L $ALICE/geant3/TGeant3/G3GUI.C |
88 | G3GUI() | |
89 | ||
6570c14d | 90 | ============================================================ |
91 | How to check the Geometry with the new Geometrical modeler | |
92 | ftp://root.cern.ch/root/doc/chapter16.pdf | |
93 | http://agenda.cern.ch/fullAgenda.php?ida=a05212 | |
94 | ============================================================ | |
95 | gAlice->Init("$ALICE_ROOT/MUON/Config.C"); | |
96 | gGeoManager->GetMasterVolume()->Draw(); | |
97 | ||
02d8f072 | 98 | |
7985603c | 99 | ============================================================ |
100 | How to run MUONdisplay | |
101 | ============================================================ | |
1eccde20 | 102 | First you need to perform a full simulation: |
7985603c | 103 | generation, digitalisation and clusterisation |
cd0f8cc8 | 104 | To run MUONdisplay with Root 5.04/00 you need to get a fix in |
105 | the gpad/src/TPad.cxx from Root CVS: | |
106 | cvs update -r 1.200 gpad/src/TPad.cxx | |
107 | and recompile root. | |
108 | ||
7985603c | 109 | .L $ALICE_ROOT/MUON/MUONdisplay.C |
110 | MUONdisplay(0,"galice.root") | |
111 | ||
02d8f072 | 112 | ============================================================ |
113 | Tracking parameters, cuts, energy loss and physics processes | |
114 | ============================================================ | |
115 | Tracking parameters in MUON are automatically defined by GEANT | |
116 | MUON takes the default values of CUTs and physics processes | |
117 | defined by the Config files, except for the gas mixture medium | |
118 | of the tracking chambers. The CUT's and physics processes of | |
119 | the gas mixture medium is then defined in the galice.cuts file | |
120 | in the data directory. In particular ILOSS parameter MUST be | |
121 | equal unity (1) in order simulate a realistic energy loss | |
122 | distribution (mean value and fluctuations) in the active gas. | |
a88eb0d0 | 123 | |
124 | ============================================================ | |
125 | Tracking of particle in the magnetic field | |
126 | ============================================================ | |
127 | GEANT has two ways for tracking charged particles in the | |
128 | magnetic field: HELIX et RKUTA. | |
129 | HELIX is faster and works well if the gradient of magnetic | |
130 | field is small. | |
131 | For MUON, HELIX is a not a good approximation and we must | |
132 | use RKUTA to get the optimal mass resolution of the | |
133 | spectrometer. The choice of HELIX or RKUTA is done in the | |
134 | config file when the magnetic field is defined: | |
135 | AliMagFMaps* field = new AliMagFMaps("Maps","Maps", TRACKING, FACTOR, MAXB, AliMagFMaps::k4kG); | |
136 | gAlice->SetField(field); | |
137 | TRACKING must be 1 for RKUTA and 2 for HELIX (the default value for aliroot is 2 (HELIX)) | |
138 | FACTOR allows you to set the magnetic field to 0, just putting FACTOR=0. Default value is 1. | |
139 | MAXB is the maximum magnetic field which is 10.T | |
2b32c661 | 140 | |
f4f795ed | 141 | =========================================================== |
142 | MUON cocktail for physics .............. | |
143 | =========================================================== | |
144 | There is a MUON cocktail generator of the muon sources in the | |
145 | EVGEN directory. This class derives from AliGenCocktail. | |
146 | In the init of this class I have filled the cocktail with | |
147 | the muon sources: J/Psi, Upsilon, Open Charm, Open Beauty, | |
148 | Pion, Kaons. The code needs only the production cross section | |
149 | at 4pi (for the moment this values are in the code since I | |
150 | prefere them do not be modified), and the code calculates the | |
151 | rate of particles in the acceptance, making the scaling based | |
152 | on the number of collisions for the hard probes and on the | |
153 | number of participants for soft sources: Pions and Kaons. | |
154 | ||
155 | In the Genereate of this class all entries in the cocktail | |
156 | are called and we define a "primordial trigger" with requires | |
157 | a minimum number of muons above a Pt cut in the required acceptance. | |
158 | In order to normalized to the real number of simulated events, | |
159 | there are 2 data members in the class fNsuceeded adn fNGenerate | |
160 | which tell us what is the biais source. | |
161 | ||
162 | Enclose an example to use this generator: | |
163 | AliGenMUONCocktail * gener = new AliGenMUONCocktail(); | |
164 | gener->SetPtRange(1.,100.); // Transverse momentum range | |
165 | gener->SetPhiRange(0.,360.); // Azimuthal angle range | |
166 | gener->SetYRange(-4.0,-2.4); | |
167 | gener->SetMuonPtCut(1.); | |
168 | gener->SetMuonThetaCut(171.,178.); | |
169 | gener->SetMuonMultiplicity(2); | |
35e21dec | 170 | gener->SetImpactParameterRange(0.,5.); // 10% most centra PbPb collisions |
f4f795ed | 171 | gener->SetVertexSmear(kPerTrack); |
172 | gener->SetOrigin(0,0,0); // Vertex position | |
173 | gener->SetSigma(0,0,0.0); // Sigma in (X,Y,Z) (cm) on IP position | |
174 | gener->Init(); | |
175 | ||
a2da7817 | 176 | ================================================================ |
69be760c | 177 | csh Script for the full reconstruction with raw data generator |
a2da7817 | 178 | ================================================================ |
179 | The rawdata generation and analysis is working with the new segmentation. | |
180 | So the config file must use the version "AliMUONFactoryV3" | |
181 | ||
182 | Generation | |
183 | The method AliSimulation::SetWriteRawData("MUON") enables on | |
184 | the muon rawdata generation | |
185 | aliroot -b << EOF | |
186 | AliSimulation MuonSim("$ALICE_ROOT/MUON/Config.C") | |
187 | MuonSim.SetWriteRawData("MUON") | |
188 | MuonSim.Run(10) | |
189 | .q | |
190 | EOF | |
191 | ||
192 | Reconstruction | |
193 | aliroot -b << EOF | |
194 | AliReconstruction MuonRec("galice.root"); | |
195 | MuonRec.SetInput("$YOUR_WORKING_DIRECTORY/"); Do not forget the slash at the end! | |
196 | MuonRec.SetRunVertexFinder(kFALSE); | |
197 | MuonRec.SetRunLocalReconstruction("MUON"); | |
198 | MuonRec.SetRunTracking(""); | |
199 | MuonRec.SetFillESD("MUON"); | |
9ffe3ef4 | 200 | MuonRec.SetOption("MUON", "AZ Kalman"); // to use AZ clustering and Kalman filter |
a2da7817 | 201 | MuonRec.Run(); |
202 | .q | |
203 | EOF | |
204 | ||
a88eb0d0 | 205 | |
b8dc484b | 206 | |
207 | ============================================================ | |
208 | How to run MUONRecoCheck macro | |
209 | ============================================================ | |
210 | To check the muon reconstruction by comparing the reconstructed tracks | |
211 | with the reference tracks made of "AliTrackReference" for the hits and | |
212 | kinematic informations (TParticle) for the vertex. | |
213 | This macro can be used to check the track reconstruction e.g. efficiency, | |
214 | momentum resolution ... but also to make physics analysis whenever | |
215 | track identification is needed. | |
216 | ||
217 | To compile MUONRecoCheck.C | |
218 | .includepath $ALICE_ROOT/STEER | |
219 | .includepath $ALICE_ROOT/MUON | |
220 | .L $ALICE_ROOT/MUON/MUONRecoCheck.C+ | |
221 | ||
222 | // To run MUONRecoCheck | |
223 | MUONRecoCheck(nEvent,"galice.root"); // nEvent = nb of events | |
224 | ||
29fc2c86 | 225 | |
226 | ============================================================ | |
227 | How to run MUONTracker macro | |
228 | ============================================================ | |
229 | To make the track reconstruction directly from AliTrackReference hits | |
230 | which are recorded in TrackRefs.root during the simulation. | |
231 | It can be used to check the reconstruction without clusterization. | |
232 | ||
233 | To compile MUONTracker.C | |
234 | .includepath $ALICE_ROOT/STEER | |
235 | .includepath $ALICE_ROOT/MUON | |
236 | .L $ALICE_ROOT/MUON/MUONTracker.C+ | |
237 | ||
238 | // To run MUONTracker | |
239 | MUONTracker(iEventMin,iEventMax,"galice.root"); // iEventMin: first event | |
fc1fafa5 | 240 | |
241 | =========================================================== | |
242 | Macro MUONGenerateGeometryData.C | |
243 | =========================================================== | |
244 | ||
245 | Macro for generating the geometry data files: | |
246 | (transform_*.dat, svmap_*.dat). | |
247 | - MUON/data/transform_*dat files contain all the information | |
248 | about the transformation (traslation + rotation) needed for | |
249 | the positionning of each detection element of the MUON | |
250 | spectrometer. | |
251 | - MUON/data/svmap_*.dat files contain all the information to link | |
252 | each geant volume (it can be extended to other virtual MC) with | |
253 | a detection element. The point here is that a given detection | |
254 | element, i.e. a slat chamber consists of many geant volumes. | |
255 | the correspondence is then defined in an input file. | |
256 | Eanch time there is a change in the virtual MC geometry, these | |
257 | input files must be re-generated via the macro | |
258 | MUONGenerateGeometryData.C | |
259 | ||
260 | To be run from aliroot: | |
261 | .x MUONGenerateGeometryData.C | |
262 | ||
263 | The generated files do not replace the existing ones | |
264 | but have different names (with extension ".out"). | |
265 | To compare/replace the existing files with generated ones | |
266 | run the scripts in MUON/data: | |
504a69a4 | 267 | compare_data.sh [transform] [svmap ] |
268 | reset_data.sh [transform] [svmap ] | |
fc1fafa5 | 269 | Author: I. Hrivnacova, IPN Orsay |
29fc2c86 | 270 | |
271 | ||
88cb7938 | 272 | =========================================================== |
273 | Still working .............. | |
274 | =========================================================== |