GEANT4 Workshop 2001 HARP and GEANT4 1 & Pedro Arce (CERN/IFCA-Santander) Vladimir Ivantchenko (CERN/Budker Institute) GEANT4 Workshop 5th July 2001.

Slides:



Advertisements
Similar presentations
HARP Anselmo Cervera Villanueva University of Geneva (Switzerland) K2K Neutrino CH Meeting Neuchâtel, June 21-22, 2004.
Advertisements

Use of G EANT 4 in CMS AIHENP’99 Crete, April 1999 Véronique Lefébure CERN EP/CMC.
Hall D Photon Beam Simulation and Rates Part 1: photon beam line Part 2: tagger Richard Jones, University of Connecticut Hall D Beam Line and Tagger Review.
Neutrino-CH 19 October 2006 Alain Blondel HARP and K2K 1. The K2K experiments 2. beam related uncertainties 3. HARP and results 4. K2K and results 5. conclusions.
Beamline Takashi Kobayashi 1 Global Analysis Meeting Nov. 29, 2007.
25/03/2003Simulation Application for the LHCb Experiment CHEP March 2003 Presented by: W. Pokorski / CERN Authors: I. Belyaev, Ph. Charpentier,
1 Analysis code for KEK Test-Beam M. Ellis Daresbury Tracker Meeting 30 th August 2005.
August 98 1 Jürgen Knobloch ATLAS Software Workshop Ann Arbor ATLAS Computing Planning ATLAS Software Workshop August 1998 Jürgen Knobloch Slides also.
LBNE R&D Briefing May 12, 2014 LBNE R&D Briefing May 12, 2014 LArIAT and LBNE Jim Stewart LArIAT EPAG Chair BNL LBNE LARIAT-EPAG J. Stewart BNL T. Junk.
Emittance measurement: ID muons with time-of-flight Measure x,y and t at TOF0, TOF1 Use momentum-dependent transfer matrices to map  path Assume straight.
Medium heavy Λ hyper nuclear spectroscopic experiment by the (e,e’K + ) reaction Graduate school of science, Tohoku University Toshiyuki Gogami for HES-HKS.
HARP for MiniBooNE Linda R. Coney Columbia University DPF 2004.
E906/Drell-Yan: Monte Carlo, Data Acquisition and Data Analysis Paul E. Reimer Expected Rates and Monte Carlo (WBS 2.5.1) Data Acquisition (WBS 2.4) –CODA.
TWIST Measuring the Space-Time Structure of Muon Decay Carl Gagliardi Texas A&M University TWIST Collaboration Physics of TWIST Introduction to the Experiment.
Status of the Beamline Simulation A.Somov Jefferson Lab Collaboration Meeting, May 11, 2010.
Status and Prospects of HARP Malcolm Ellis On behalf of the HARP Collaboration NuFact02 Imperial College, July 2002.
Track Reconstruction: the trf & ftf toolkits Norman Graf (SLAC) ILD Software Meeting, DESY July 6, 2010.
DE/dx measurement with Phobos Si-pad detectors - very first impressions (H.P Oct )
The BESIII Offline Software Weidong Li Institute of High Energy Physics, Beijing Workshop on the cooperation of PRC-US in HEP 16 June 2006.
TWIST A Precision Measurement of Muon Decay at TRIUMF Peter Kitching TRIUMF/University of Alberta TWIST Collaboration Physics of TWIST Introduction to.
BeamCal Simulations with Mokka Madalina Stanescu-Bellu West University Timisoara, Romania Desy, Zeuthen 30 Jun 2009 – FCAL Meeting.
The East Area Rende Steerenberg, ps/op PS-Days 2001 Evian.
Detector Simulation Presentation # 3 Nafisa Tasneem CHEP,KNU  How to do HEP experiment  What is detector simulation?
Magnetic Field Issues for Simulation and Reconstruction N. Amapane, N. Neumeister Workshop on LHC Physics with High-p T Muons in CMS Bologna, April 9-12,
1 Energy loss correction for a crystal calorimeter He Miao Institute of High Energy Physics Beijing, P.R.China.
8 June 2006V. Niess- CALOR Chicago1 The Simulation of the ATLAS Liquid Argon Calorimetry V. Niess CPPM - IN2P3/CNRS - U. Méditerranée – France On.
CALICE Digital Hadron Calorimeter: Calibration and Response to Pions and Positrons International Workshop on Future Linear Colliders LCWS 2013 November.
22 September 2005 Haw05 1  (1405) photoproduction at SPring-8/LEPS H. Fujimura, Kyoto University Kyoto University, Japan K. Imai, M. Niiyama Research.
1 Mariyan Bogomilov CERN,(Switzerland) University of Sofia and INRNE, (Bulgaria) Kiten, Bulgaria THE HARP EXPERIMENT THE HARP EXPERIMENT.
Detector Monte-Carlo ● Goal: Develop software tools to: – Model detector performance – Study background issues – Calculate event rates – Determine feasibility.
The CMS Simulation Software Julia Yarba, Fermilab on behalf of CMS Collaboration 22 m long, 15 m in diameter Over a million geometrical volumes Many complex.
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.
Muon Reconstruction with Moore and MuonIdentification The Moore/MUID group Atlas Physics Workshop Athens, May 2003.
Geant4 Simulation of the Beam Line for the HARP Experiment M.Gostkin, A.Jemtchougov, E.Rogalev (JINR, Dubna)
Particle Identification at BESIII Kanglin He April 23, 2007, Amsterdam.
Detector Description in LHCb Detector Description Workshop 13 June 2002 S. Ponce, P. Mato / CERN.
HARP measurements of pion yield for neutrino experiments Issei Kato (Kyoto University) for the HARP collaboration Contents: 1.HARP experiment Physics motivations.
Dual Target Design for CLAS12 Omair Alam and Gerard Gilfoyle Department of Physics, University of Richmond Introduction One of the fundamental goals of.
26 Oct 2010PC Physics Requirements of Software from Chris R ~19 Oct. My.
GLAST LAT Project CU Beam Test Workshop 3/20/2006 C. Sgro’, L. Baldini, J. Bregeon1 Glast LAT Calibration Unit Beam Test Status Report on Online Monitor.
Geant4 CPU performance : an update Geant4 Technical Forum, CERN, 07 November 2007 J.Apostolakis, G.Cooperman, G.Cosmo, V.Ivanchenko, I.Mclaren, T.Nikitina,
Status of Sirene Maarten de Jong. What?  Sirene is yet another program that simulates the detector response to muons and showers  It uses a general.
H A R P A Hadron Production Experiment at the Proton Synchrotron at CERN Motivation for the HARP experiment The HARP Detector MiniBooNE and HARP.
Mu to e Meeting BNL, June 2006 Extinction requirement relaxation (Kevin O’Sullivan) Stopping Target Geometry (Cenap Ozben, David Morse) Yannis Semertzidis.
STAR Simulation. Status and plans V. Perevoztchikov Brookhaven National Laboratory,USA.
P.F.Ermolov SVD-2 status and experimental program VHMP 16 April 2005 SVD-2 status and experimental program 1.SVD history 2.SVD-2 setup 3.Experiment characteristics.
A. SarratILC TPC meeting, DESY, 15/02/06 Simulation Of a TPC For T2K Near Detector Using Geant 4 Antony Sarrat CEA Saclay, Dapnia.
A New Upper Limit for the Tau-Neutrino Magnetic Moment Reinhard Schwienhorst      ee ee
ATLAS The ConditionDB is accessed by the offline reconstruction framework (ATHENA). COOLCOnditions Objects for LHC The interface is provided by COOL (COnditions.
BESIII offline software group Status of BESIII Event Reconstruction System.
Object-Oriented Track Reconstruction in the PHENIX Detector at RHIC Outline The PHENIX Detector Tracking in PHENIX Overview Algorithms Object-Oriented.
A Short Course on Geant4 Simulation Toolkit Introduction
CHEP ’06 GEANT4E 1 GEANT4E: Error propagation for track reconstruction inside the GEANT4 framework Pedro Arce (CIEMAT) CHEP 2006, Mumbai, 13-17th February.
(one of the) Request from MPB
Track Reconstruction: the ftf and trf toolkits Norman Graf (SLAC) Common Software Working Meeting CERN, January 31, 2013.
Monthly video-conference, 18/12/2003 P.Hristov1 Preparation for physics data challenge'04 P.Hristov Alice monthly off-line video-conference December 18,
SPSC, 26 March 2002 A. De Min, HARP STATUS REPORT 1 HARP STATUS REPORT A. De Min for the HARP Collaboration SPSC Open Session 26 March 2002.
Background simulations: update and simulations of absorbed dose
Simulation Tools for Test Beam
Measurement of track length and time-of-flight hypothesis
Commissioning of the ALICE HLT, TPC and PHOS systems
Summary of hadronic tests and benchmarks in ALICE
(CMS GEANT4 simulation)
Preparation of the CLAS12 First Experiment Status and Time-Line
Use of Geant4 in experiment interactive frameworks AliRoot
A Short Course on Geant4 Simulation Toolkit Introduction
EEE telescope simulation
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
ACCELERATORS AND DETECTORS
release 5.0 – planned features
Presentation transcript:

GEANT4 Workshop 2001 HARP and GEANT4 1 & Pedro Arce (CERN/IFCA-Santander) Vladimir Ivantchenko (CERN/Budker Institute) GEANT4 Workshop 5th July 2001

GEANT4 Workshop 2001 HARP and GEANT4 2 HARP will measure Hadronic production cross sections (d  /dP t.dP l ) at various energies and with various targets Goal: 2% accuracy over all phase space O(10 6 ) events/setting, low systematic error Current Run (2001): CERN PS, T9 beam: 2 GeV/c – 15 GeV/c protons, pi -, pi +, K -, K + Targets: Be, C, Al, Cu, Fe, Pb, W (thin and thick) Measurements with solid and cryogenic targets, 2001 Future plans: Measurements with incoming Deuterium and Helium, 2002 ~100 GeV incoming beam, using NA49 set-up

GEANT4 Workshop 2001 HARP and GEANT4 3 Deliverables Input data for the design of the Neutrino factory/Muon collider Input data for the Atmospheric neutrino flux calculations Precise predictions of the neutrino fluxes for the K2K and MiniBooNE experiments Input data for the hadron generators in Monte Carlo simulation packages

GEANT4 Workshop 2001 HARP and GEANT4 4 Experimental setup drift chambers cherenkov TOF wall electron identifier spectrometer magnet TPC solenoid magnet forward trigger forward RPC muon identifier beam

GEANT4 Workshop 2001 HARP and GEANT4 5 Experimental setup

GEANT4 Workshop 2001 HARP and GEANT4 6 p/  separation TPC TOF Cherenkov p/  separation at 4  level, “conservative” simplification Pt-Pl box plot of  distribution from 15 GeV p on Be thin target

GEANT4 Workshop 2001 HARP and GEANT4 7 Stringent time schedule required adoption of software engineering standards. Software deliverables for the Technical Run: –Project and Configuration Management Plans –User and Software Requirements Documents –Architectural Design Document & Design Diagrams –Test Plan and Release Procedures –Traceability matrixes across software deliverables Domains identification & dependency structure lead to: –definition of releasable units (libraries and source code), –definition of working groups (and schedules), –definition of ordering for unit&system testing and for release. Software Process

GEANT4 Workshop 2001 HARP and GEANT4 8 DAQ and detectors readout (DATE). Storage and retrieval of physics data and settings (Objectivity DB, AMS-HPSS interface). Framework including application manager, interfaces & data exchange for the components, and event model (GAUDI). Physics Simulation & Detector Model (GEANT4). Physics Reconstruction for DC data. Online Monitoring & Offline Calibration of detectors. User Interface and Event Display (ROOT). Foundation libs & Utilities (STL, CLHEP). Software Functionality

GEANT4 Workshop 2001 HARP and GEANT4 9 Software architecture

GEANT4 Workshop 2001 HARP and GEANT4 10 4From ASCII files based on a few tags uDefine a single logical volume (solid and material): VOLU :VOLU "TPC" "TUBE" "Air" uDefine a logical volume made up of a substraction (addition, intersection) of two volumes: VOLU_SUBS(_ADD/_INTERS) :VOLU_SUBS "Tpc Gas" "Tpc Gas1" "Tpc Gas2" "RM0" uSingle positioning: POS :POS "Tpc Gas" 1 "TPC" "RM0" :ONLY uReplica: DIV_NUM / DIV_STEP :DIV_NUM "PAD sector" "PAD support" "Epoxy" 6 "PHI” uPositioning with a parameterisation: POS_PARAM (only a few available) Change position at each copy Change rotation at each copy :POS_PARAM "PAD" 1 "PAD sector" "CIRCLE" $n uSet visibility of a logical volume: VIS :VIS "PAD" OFF uSet the RGB colour of a logical volume: COLOUR/:COLOR :COLOUR "PAD" Geometry Description

GEANT4 Workshop 2001 HARP and GEANT4 11 uDefine rotation matrices: ROTM :ROTM "RM0" uMaterials Define an element: ELEM :ELEM "Fluorine" "F" Define a simple material (1 element): MATE :MATE "Aluminium" Define a mixture (made of elements or materials): MIXT –by weight fractions –by number of atoms –by volume :MIXT "Air" 1.214e-3 4 "Nitrogen" "Oxygen" "Argon" "Hydrogen" Geometry Description (II)

GEANT4 Workshop 2001 HARP and GEANT4 12 uGeneric representation independent GEANT4 uGEANT4 representation –access all data from the generic representation uDigitisation / Reconstruction –ask GEANT4 representation for the volumes they need (by name) HdrGeometryMgr::getInstance()->getTouchables(“TpcSector#2/TpcPad#12”)  return GEANT4 independent representation: touchables and logical volumes uVisualisation (ROOT) –ask generic representation, except replicated and parameterised positionings, where it asks GEANT4  builds ROOT representation Geometry Representations

GEANT4 Workshop 2001 HARP and GEANT4 13 Software architecture Reconstruction Digitisation Simulation GEANT4 Geometry Detector Description ROOT Visualisation Framework (GAUDI)

GEANT4 Workshop 2001 HARP and GEANT4 14 uTakes care of: –Primary generator –Physics list –User actions uGEANT4 geometry representation is in another package  Reconstruction/visualisation can use GEANT4 geometry without initialising G4RunManager uTwo magnetic field maps parameterised uThree PrimaryGenerators available allowed –HarpGun, G4GeneralParticleSource, T9 beam generator uMultiple run/event/stacking/tracking/stepping actions allowed –one action registered to GEANT4, that loops to the actions registered to it uGEANT4 event loop managed by GAUDI event loop –each event is simulated then reconstructed GEANT4 simulation

GEANT4 Workshop 2001 HARP and GEANT4 15  What it does: Needed for track reconstruction:  Start with an initial track state (energy, position and direction with their errors) in some subdetector  GEANT4e: calculates the track state in another surface of the detector  How it does it:  Propagates average trajectory  Computes average energy loss (positive or negative)  Propagates errors:  Propagates errors along the trajectory  Adds fluctuation in multiple scattering  Adds fluctuation in energy loss  Adds errors of magnetic field GEANT4 error propagator

GEANT4 Workshop 2001 HARP and GEANT4 16  Status:  Uses G4Transportation to propagate from an initial track state to a user defined surface (infinite plane) in the  GEANT4 geometry  GEANT4 magnetic field  Propagates errors in case of no magnetic field (linear trajectory)  Plans  Propagate errors in magnetic field for different trajectory representations  Assume helix trajectory?  Calculate errors of RungeKutta? GEANT4 error propagator

GEANT4 Workshop 2001 HARP and GEANT4 17 All geometry described Magnetic field described (parameterised) Physics list electromagnetic and hadronic Digitisation implemented for two main subdetectors (Tracking Projection Chamber and Drift Chambers)  Work on progress for digitisation of other subdetectors Reconstruction in DC and TPC using GEANT4: –error propagator (GEANT4e) –simulated events for debugging Status of GEANT4 simulation

GEANT4 Workshop 2001 HARP and GEANT4 18 HARP with GEANT4

GEANT4 Workshop 2001 HARP and GEANT4 19  No real data before july 2001  Reconstruction and analysis software not ready before end of year  Several thousands of events produced  No need of mass production of simulated events before a few months  No results of cross sections for GEANT4 before six months Status of GEANT4 simulation (II)