Overview Maurizio Ungaro 1HPS Collaboration meetingOctober 19 2011 Status, Future of GEMC.

Slides:



Advertisements
Similar presentations
Cheikh Anta Diop University, Dakar (SENEGAL)
Advertisements

Use of G EANT 4 in CMS AIHENP’99 Crete, April 1999 Véronique Lefébure CERN EP/CMC.
Parameterized Shower Simulation in Lelaps: a Comparison with Geant4 Daniel Birt, Amy Nicholson.
Thomas Jefferson National Accelerator Facility Page 1 Internal Software Review Jefferson Lab November 6-7, 2014 Hall B:User Software Contributions Gerard.
Simulation of the spark rate in a Micromegas detector with Geant4 Sébastien Procureur CEA-Saclay.
F ERMILAB T EST B EAM F ACILITY Aria Soha March 17, 2011.
Software Simulation of Electronics Readout Chain for the Silicon Vertex Tracker Department of Physics, University of New Hampshire, Durham, NH, Daniel.
Luminosity Monitor Commissioning MICE Collaboration Meeting March 2010 Paul Soler, David Forrest Danielle MacLennan.
Track Timing at e + e - Linear Collider with the Silicon Drift Detector Main Tracker R. Bellwied, D. Cinabro, V. L. Rykov Wayne State University Detroit,
October 20th, 2006 A. Mazzacane 1 4 th Concept Software First Results.
14 Overview of Geant4 Examples 2 nd Finnish Geant4 Workshop 6-7 June 2005 Dennis Wright (SLAC)
Study of two pion channel from photoproduction on the deuteron Lewis Graham Proposal Phys 745 Class May 6, 2009.
17-19 Oct, 2007Geant4 Japan Oct, 2007Geant4 Japan Oct, 2007Geant4 Japan 2007 Geant4 Japan.
A Short Guide to Choosing a Physics List Geant4 Tutorial at Marshall Space Flight Center 19 April 2012 Dennis Wright (SLAC) Geant4 9.5.
The Design of a Detector for the Electron Relativistic Heavy Ion Collider Anders Ingo Kirleis 1, William Foreman 1, Elke-Caroline Aschenauer 2, and Matthew.
I have made the second half of the poster, first half which is made by tarak will have neutrino information. A patch between the two, telling why we do.
CLAS12 CalCom Activity CLAS Collaboration Meeting, March 6 th 2014.
SoLID Simulation Zhiwen Zhao 赵志文 University of Virginia 2011/8/9
User Documents and Examples I Sébastien Incerti Slides thanks to Dennis Wrigth, SLAC.
HPS Online Software Discussion Jeremy McCormick, SLAC Status and Plans.
SoLID Simulation Zhiwen Zhao UVa Hall A Collaboration Meeting 2011/6/10 1 Introduction Simulation framework Simulation study Introduction Simulation framework.
SuperNEMO Simulations Darren Price University of Manchester July, 2005.
Implementing a dual readout calorimeter in SLIC and testing Geant4 Physics Hans Wenzel Fermilab Friday, 2 nd October 2009 ALCPG 2009.
Reaction plane reconstruction1 Reaction plane reconstruction in extZDC Michael Kapishin Presented by A.Litvinenko.
Updating JUPITER framework using XML interface Kobe University Susumu Kishimoto.
SoLID simulation Zhiwen Zhao Uva SoLID Collaboration Meeting 2011/6/2 1.
CLAS12 Simulation Analysis and Optimization K.Dergachev and G.P.Gilfoyle University Of Richmond - Department of Physics Introduction Jefferson Laboratory.
LAV Software Status Emanuele Leonardi – Tommaso Spadaro Photon Veto WG meeting – 2015/03/24.
Computing Performance Recommendations #13, #14. Recommendation #13 (1/3) We recommend providing a simple mechanism for users to turn off “irrelevant”
Preliminary results with the Alibava Telescope G. Casse, S. Martì, J. Rodriguez, I. Tsurin and the Alibava collaboration 1 G. Casse,20th RD50 Workshop,
Hadronic Interaction Studies for LHCb Nigel Watson/Birmingham [Thanks to Silvia M., Jeroen v T.]
Luminosity Monitor UKNF Meeting 7 June 2010 Paul Soler, David Forrest Danielle MacLennan.
Călin Alexa, CERN, July /8 ATLAS Tilecal: pion – proton comparison C. Alexa, S. Constantinescu, S. Dita 2002 test-beam data QGSP 2.7 LHEP 3.6 Groom.
1 Status and Plans for Geant4 Physics Linear Collider Simulation Workshop III 2-5 June 2004 Dennis Wright (SLAC)
CEBAF The Continuous Electron Beam Accelerating Facility(CEBAF) is the central particle accelerator at JLab. CEBAF is capable of producing electron beams.
F ERMILAB T EST B EAM F ACILITY Aria Soha March 22, 2011.
Feb. 7, 2007First GLAST symposium1 Measuring the PSF and the energy resolution with the GLAST-LAT Calibration Unit Ph. Bruel on behalf of the beam test.
Latifa Elouadrhiri Jefferson Lab Hall B 12 GeV Upgrade Drift Chamber Review Jefferson Lab March 6- 8, 2007 CLAS12 Drift Chambers Simulation and Event Reconstruction.
Thomas Jefferson National Accelerator Facility Page Hall B:User Software Contributions Gerard Gilfoyle University of Richmond 12 GeV Upgrade Software Review.
CEBAF The Continuous Electron Beam Accelerating Facility (CEBAF) at JLab in Newport News, Virginia, is used to study the properties of quark matter. CEBAF.
1 Background radiation studies in LHCb with GAUSS/Geant4 Giuseppe G. Daquino PH/SFT.
Cristian Bungau ThorEA Meeting - Oxford - April 2010.
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #15.
SoLID simulation with GEMC Zhiwen Zhao 2015/03/26.
The Compact Muon Solenoid. What does CMS do? The Compact Muon Solenoid is a general purpose particle detector installed at point 5 of the Large Hadron.
CMS H4 ECAL testbeam data comparison with simulation F.Cossutti a), B. Heltsey b), P. Meridiani c), C. Rovelli c) a) INFN Trieste b) Cornell University.
SoLID simulation Zhiwen Zhao UVa 2011/03/25 1. GEMC, written by Maurizio Ungaro, used for CLAS12 2.
Dual Target Design for CLAS12 Omair Alam and Gerard Gilfoyle Department of Physics, University of Richmond Introduction One of the fundamental goals of.
Inclusive Measurements of inelastic electron/positron scattering on unpolarized H and D targets at Lara De Nardo for the HERMES COLLABORATION.
T. Lari – INFN Milan Status of ATLAS Pixel Test beam simulation Status of the validation studies with test-beam data of the Geant4 simulation and Pixel.
1 Hadronic calorimeter simulation S.Itoh, T.Takeshita ( Shinshu Univ.) GLC calorimeter group Contents - Comparison between Scintillator and Gas - Digital.
F ERMILAB T EST B EAM F ACILITY Aria Soha June 12, 2012.
Marina Golubeva, Alexander Ivashkin Institute for Nuclear Research RAS, Moscow AGeV simulations with Geant4 and Shield Geant4 with Dpmjet-2.5 interface.
1 Giuseppe G. Daquino 26 th January 2005 SoFTware Development for Experiments Group Physics Department, CERN Background radiation studies using Geant4.
Feb. 3, 2007IFC meeting1 Beam test report Ph. Bruel on behalf of the beam test working group Gamma-ray Large Area Space Telescope.
Study of Calorimeter performance using the LC full simulator The 8th ACFA Workshop Yoshihiro Yamaguchi (Tsukuba U.) M. -C. Chang (RCNS, Tohoku U.) K. Fujii.
FEE for Muon System (Range System) Status & Plans G.Alexeev on behalf of Dubna group Turin, 16 June, 2009.
Simulation and reconstruction of CLAS12 Electromagnetic Calorimeter in GSIM12 S. Stepanyan (JLAB), N. Dashyan (YerPhI) CLAS12 Detector workshop, February.
The MiniBooNE Little Muon Counter Detector
Stress tests for CLAS12 software
Testbeams for Simulation
Overview of CLAS12 Calibration
SoLID Simulation Zhiwen Zhao 2016/08/27.
QGSP_BERT和 QGSP.
The n-3He Simulation Using Geant4
SoLID simulation with GEMC
CLAS Simulations for the E5 Data Set
SoLID Simulation Zhiwen Zhao (UVa) SoLID Jlab Physics Division
The n-3He Simulation Using Geant4
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
Presentation transcript:

Overview Maurizio Ungaro 1HPS Collaboration meetingOctober Status, Future of GEMC

GEMC (GEant4 MonteCarlo) gemc is a C++ program that simulates particles through matter using the geant4 libraries. 2HPS Collaboration meetingOctober

GEMC (GEant4 MonteCarlo) gemc is a C++ program that simulates particles through matter using the geant4 libraries. 3HPS Collaboration meetingOctober GEOMETRY, BANKS, DIGITIZATION DATABASE gemc

GEMC (GEant4 MonteCarlo) gemc is a C++ program that simulates particles through matter using the geant4 libraries. 4HPS Collaboration meetingOctober gemc FTOF Panels DC: R3 R2 R1 DC: R3 R2 R1 CLAS12 Torus HTCC Mirrors Tubes HTCC Mirrors Tubes PCAL Baffles Solenoid GAS Cerenkov ECAL Magnetic Chicane Silicon Tracker

GEMC (GEant4 MonteCarlo) 5HPS Collaboration meetingOctober gemc ECAL Magnetic Chicane Silicon Tracker Advantages: User: Change parameters w/o touching the code: very fast R/D and deployment Abstract Objects instantiated thousands of times ensures they are “correct”: “can’t” make a mistake Can make “alignment, kinematic fit” on the fly (tilts, shifts) No need to know C++ or Geant4 Development: Easy to debug (table  reproducibility) Can concentrate on “core” code.

Factory Method for Hit Processes Hit Process, Digitizations External Routines CTOF gemc DC SVT gemc FTOF Automatic Process Routines Still External Easy to: add new routine debug modify 6HPS Collaboration meetingOctober

Output (factory) TXT output: -OUTPUT=“txt, data.txt” EVIO OUTPUT: -OUTPUT=“evio, data.ev” 7HPS Collaboration meetingOctober

Event Generation 1)With gemc internal generator 2)LUND Format for physics events: To all these “primary” particles, a luminosity beam can be added 8HPS Collaboration meetingOctober

Luminosity Beam 9HPS Collaboration meetingOctober Number of Beam Particle / One single Event Time Window of the event Time Structure of the Event: “bunches” time separation 8000 electrons / event 1 event = 16 nanoseconds Bunches every 2 nanoseconds (8 bunches, 1000 electron each bunch) Physics event generated in the middle (8 ns)

Physics Processes Databases LHEP Physics Lists The LHEP Physics lists are based on a parameterized modeling for all hadronic interactions for all particles.Based on Geisha model. Example: LHEP_BERT (Bertini Cascade) String model based physics lists These Physics lists apply a string models for the modeling of interactions of high energy hadrons, i.e. for protons, neutrons, pions and Kaons above ~(5-25) GeV. Examples: QGSP: quark gluon string model QGSC: CHIPS modeling for the nuclear de-excitation QGSC_BERT: Bertini cascade for primary protons, neutrons, pions and Kaons below ~10GeV. (recommended for CLAS12) 10HPS Collaboration meetingOctober

Optical Processes in GEMC HPS Collaboration meeting11October

Physics Processes Databases Future: factory process 12HPS Collaboration meetingOctober Model the physics processes in the external database: Can turn on/off single processes for all/individual particles (very useful for eg5 comparison and debugging in general) Can modify energy range of applicability of processes (e.g. Bertini cascade model, Low energy parameterization, etc)

1)“FLUX” type: every track has its own hit. Good for counting purposes (i.e. how many protons pass through a detector, etc) Hit Types Databases Primary track 2 Primary track 1 Secondary 1 Secondary 2 2) Time Window ADC: all hits (separate tracks too) in the same time window for a particular detector will be added to a single hit Sense Wire 3) Time Window TDC: the first signal within the detector time window will give the TDC. 13HPS Collaboration meetingOctober ) Signal Modeling: Real Voltage Response to passage of Particles

Hit Types Databases 14HPS Collaboration meetingOctober Signal Modeling Parameterization: Each Scintillator, Tube, etc, modeled by a few parameters in DB Tube Association in Geometry DB (same as Hit Process): Volume X is a Bicron 408 Scintillator attached to a Amperex XP2262 Tube

Geometry Database Extension to GDML input (output is supported thanks to Maurik) Hall-D extension? LCSIM extension? 15HPS Collaboration meetingOctober

Materials Database Future: Factory Method 16HPS Collaboration meetingOctober Materials will be defined in DB GDML Extension (last hurdle to complete the code-writing independence)

Conclusion: gemc.jlab.org 17HPS Collaboration meetingOctober