28-Aug-2003 Steve Kahn Standardized MucGeant I/O Front End to MucGeant Standardize the input files for MucGeant: –The input should be in the ICOOL for003/4.

Slides:



Advertisements
Similar presentations
Preparing CMOR for CMIP6 and other WCRP Projects
Advertisements

1 Progress report on Calorimeter design comparison simulations MICE detector phone conference Rikard Sandström.
Cooling channel issues U. Bravar Univ. of Oxford 31-Mar-2004.
Summary of downstream PID MICE collaboration meeting Fermilab Rikard Sandström.
Taylor Models Workhop 20 December 2004 Exploring and optimizing Adiabatic Buncher and Phase Rotator for Neutrino Factory in COSY Infinity A.Poklonskiy.
1 Muon Yield Comparisons for Different ICOOL Versions and Lattices X. Ding Front End, Nov. 23, 2010.
March 31, Status of the TOF, Ckov and Virtual Detector Packages in G4Mice Steve Kahn Brookhaven National Laboratory Mice Collaboration Meeting March.
Chris Rogers, MICE CM16 Wednesday Plenary Progress in Cooling Channel Simulation.
Emittance Calculation Chris Rogers, Imperial College/RAL Septemebr
1Malcolm Ellis - Software Meeting - 31st May 2006 Data Challenge Requirements  First list of requirements, based on Yagmur’s document: u
 Transverse Polarization in STAR Au-Au Collisions Polarization definition and models E896 results STAR analysis STAR results Significance of results Future.
Oct 15, 2003 Video Conference Energy Deposition Steve Kahn Page 1 Energy Deposition in MICE Absorbers and Coils Steve Kahn October 15, 2003.
Helical Cooling Channel Simulation with ICOOL and G4BL K. Yonehara Muon collider meeting, Miami Dec. 13, 2004 Slide 1.
Analysis of MICE Chris Rogers 1 Imperial College/RAL Thursday 28 October, With thanks to John Cobb.
Introduction to Longitudinal Phase Space Tomography Duncan Scott.
Oct 15, 2003 Video Conference Energy Deposition Steve Kahn Page 1 Energy Deposition in MICE Absorbers and Coils Steve Kahn November 2, 2003.
Introduction Status of SC simulations at CERN
Electrical Noise Location System Drew Compston Richard Denney Josh Gordon.
Using FLUKA for radioactive waste zoning L. Nicolas, FLUKA meeting, March
June 21, 2005 S. Kahn -- Small Muon Cooling Ring1 Small Muon Ring for a Cooling Demonstration Steve Kahn For S. Kahn, H. Kirk, A. Garren, F. Mills and.
Tracking Studies of Phase Rotation Using a Scaling FFAG Ajit Kurup FFAG07 12 th – 17 th April 2007.
Mar 19, 2008 S. Kahn -- RF in HCC Channel 1 Examination of How to Put RF into the HCC Steve Kahn NFMCC Meeting Mar 19, 2008.
Feb 10, 2005 S. Kahn -- Pid Detectors in G4MicePage 1 Pid Detector Implementation in G4Mice Steve Kahn Brookhaven National Lab 10 Feb 2005.
26 Jan, MEG Software Status Framework for MEG MC, Unification of LargePrototype/beam test, Schedule and DC reconstruction MEG Software Group.
Magnet Issues Steve Kahn OleMiss Workshop Mar 11, 2004.
JLab hypernuclear collaboration meeting / JSPS Core to Core Seminar TOSCA models for ENGE and other spectrometers 9May2012 – 11May2012 Department of Physics,
Status of Scaling FFAG Phase Rotation ICOOL Simulations Ajit Kurup ISS Machine Group Meeting 27 th July 2006.
FLUKA dose and fluence simulations for CBM experiment I.Kadenko, O.Bezshyyko, V.Pluyko, V.Shevchenko National Taras Shevchenko University of Kiev.
Update Chris Rogers, Analysis PC, 13/07/06. State of the “Accelerator” Simulation Field model now fully implemented in revised MICE scheme Sanity checking.
Simulations for CBM CBM-India Meeting, Jammu, 12 February 2008 V. Friese
Eric Prebys, FNAL.  In our previous discussion, we implicitly assumed that the distribution of particles in phase space followed the ellipse defined.
Beam MC activity A.K.Ichikawa for beam group For more details,
What is in my contribution area Nick Sinev, University of Oregon.
S. Kahn 5 June 2003NuFact03 Tetra Cooling RingPage 1 Tetra Cooling Ring Steve Kahn For V. Balbekov, R. Fernow, S. Kahn, R. Raja, Z. Usubov.
Beam Loss Simulation in the Main Injector at Slip-Stacking Injection A.I. Drozhdin, B.C. Brown, D.E. Johnson, I. Kourbanis, K. Seiya June 30, 2006 A.Drozhdin.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Office of Science U.S. Department of Energy Containing a.
March 2, 2011 TJRPhysics Processes Missing from our Current Simulation Tools 1 Tom Roberts Muons, Inc. This is the current list − Please help us to complete.
Chicane simulation update Pavel Snopok Front end phone meeting January 14,
Oct 15, 2003 Video Conference Energy Deposition Steve Kahn Page 1 Energy Deposition in MICE Absorbers and Coils Steve Kahn November 2, 2003.
Geant4 Simulation of the Beam Line for the HARP Experiment M.Gostkin, A.Jemtchougov, E.Rogalev (JINR, Dubna)
1 Pad Chamber Simulation Results for Muon Trigger Upgrade 10/13/2003 Muon Trigger Upgrade meeting.
M. Ellis - MICE Collaboration Meeting - Thursday 28th October Sci-Fi Tracker Performance Software Status –RF background simulation –Beam simulation.
PID simulations Rikard Sandström University of Geneva MICE collaboration meeting RAL.
1 Virtual Accelerator plan and status at RCS Hiroshima University, Graduate School of Science Experimental Quark Physics Lab ( & JAEA Accelerator Development.
M. Ellis - MICE Video Conference - 30th August Software Report Recent progress:Recent progress: –Start of code to read DATE format (two parts) One.
Status of BDSIM Simulation L. Nevay, S. Boogert, H. Garcia-Morales, S. Gibson, R. Kwee-Hinzmann, J. Snuverink Royal Holloway, University of London 17 th.
Field Modelling Tools in G4MICE MICE VC Chris Rogers 1st Feb 2006.
By Verena Kain CERN BE-OP. In the next three lectures we will have a look at the different components of a synchrotron. Today: Controlling particle trajectories.
How to… (a.k.a. Photon PID and Pizero Analysis) G. David, April 20, 2000 A report on the status and advertisement of the tools
2 July 2002Realistic Fields for a Ring Cooler Magnet System -- S.Kahn Page 1 Realistic Fields for a Ring Cooler Steve Kahn 2 July 2002 NuFact’02 Meeting.
Update on the Status of BDSIM Steve Malton On behalf of: Grahame Blair (RHUL) Ilya Agapov (CERN) Andrea Latina (CERN) Olivier Dadoun (LAL) Anyone else.
Simulating the RFOFO Ring with Geant Amit Klier University of California, Riverside Muon Collaboration Meeting Riverside, January 2004.
1 Giuseppe G. Daquino 26 th January 2005 SoFTware Development for Experiments Group Physics Department, CERN Background radiation studies using Geant4.
STAR Simulation. Status and plans V. Perevoztchikov Brookhaven National Laboratory,USA.
Nufact02, London, July 1-6, 2002K.Hanke Muon Phase Rotation and Cooling: Simulation Work at CERN new 88 MHz front-end update on cooling experiment simulations.
1 Simulation, Formatter & Analysis Kyo Tsukada Tohoku Univ.
Tau31 Tracking Efficiency at BaBar Ian Nugent UNIVERSITY OF VICTORIA Sept 2005 Outline Introduction  Decays Efficiency Charge Asymmetry Pt Dependence.
Adiabatic buncher and (  ) Rotator Exploration & Optimization David Neuffer(FNAL), Alexey Poklonskiy (FNAL, MSU, SPSU)
Intra-Beam scattering studies for CLIC damping rings A. Vivoli* Thanks to : M. Martini, Y. Papaphilippou *
MONTE CARLO TRANSPORT SIMULATION Panda Computing Week 2012, Torino.
Object-Oriented Track Reconstruction in the PHENIX Detector at RHIC Outline The PHENIX Detector Tracking in PHENIX Overview Algorithms Object-Oriented.
Study of influence of particle identification and resonances excitation on correlation functions mesured by ALICE setup. 1. Influence of particle identification.
1 HcalAlCaRecoProducers : Producer for HO calibration Outer hadron calorimeter is expected to improve jet energy resolution Due to different sampling/passive.
Dollan, Laihem, Lohse, Schälicke, Stahl 1 Monte Carlo based studies of polarized positrons source for the International Linear Collider (ILC)
G4beamline Spin Tracking Tom Roberts, Muons, Inc. In G4beamline 2.12, the tracking of muon and electron spins is introduced: – decay of pions into polarized.
Zgoubi tracking study of the decay ring
Beam-Beam status in SixTrack (1)
Physics Processes Missing from our Current Simulation Tools
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
Geant Simulation of Muon Cooling Rings
Presentation transcript:

28-Aug-2003 Steve Kahn Standardized MucGeant I/O Front End to MucGeant Standardize the input files for MucGeant: –The input should be in the ICOOL for003/4 format: This is followed by an indefinite number of incident particles, each with the following data. –(1) IEVT(I) event #(increase sequentially from 1) –(2) IPNUM(I) particle # for this event (set to 1) –(3) IPTYP(I) particle type code (see BMTYPE in sec. 2.4) –(4) IPFLG(I) particle status flag (set to 0) –(5) TP(R) time [s] –(6) EVTWT(R) event weight (set to 1.) –(7) XP(i),i=1,3(R) cartesian position [m] (set xp(3)=0.) –(8) PP(i),i=1,3(R) cartesian momentum [GeV/c] –(9) POL(i),i=1,3(R) cartesian spin vector This would permit, for example, to us to use a file with muons generated with ICOOL for the front end to be inserted into a ring. This would permit direct comparisons with ICOOL with the same input source.

28-Aug-2003 Steve Kahn Standardized MucGeant I/O Issues associated with standardized ICOOL input file –ICOOL works in a local coordinate system around the reference orbit. GEANT works in the global coordinate system. The approach that was adapted is that one would place a virtual volume at the point of insertion into GEANT. Coordinates internal to this virtual volume would be in ICOOL local coordinates and the GEANT transformation methods would be used to get the proper global coordinates for GEANT to use. –The virtual volume description is in data cards in the RCP date file. The position of this virtual start volume is not completely arbitrary since it must be consistent with the TARGET_TIME variable in the RCP file so as to coordinate the RF timing of the cavities.

28-Aug-2003 Steve Kahn Standardized MucGeant I/O Issues (continued) –We will modify a simple utility program to write this ICOOL for003 file with Gaussian distributions around x, Px, y, Py, E, t with the proper Pt, r, B, E correlations. This utility was used for the Tetra ring input.

28-Aug-2003 Steve Kahn Standardized MucGeant I/O Output File for Analysis Since our main interest is emittance we would like to have an output format to facilitate that. We have chosen to output analysis data in the ICOOL for009 format so that it can go into ECALC9. –This would allow us to make exactly the same emittance calculation as used by ICOOL (right or wrong?) ICOOL for009 format: –This is followed by particle information at requested positions. 1) IEVT(I) event # 2) IPNUM(I) particle # for this event 3) IPTYP(I) particle type code (see BMTYPE in sec. 2.2) 4) IPFLG(I) particle status flag 5) JSRG(I) ICOOL region # 6) TP(R) time [s] 7) XP(i),i=1,3(R) position [m] 8) PP(i),i=1,3(R) cartesian momentum [GeV/c] 9) BFLD(i),i=1,3(R) total magnetic field [T] 10) EVTWT(R) event weight 11) EFLD(i),i=1,3(R) total electric field [V/m] 12) SARC(R) total arclength [m] 13) POL(i),i=1,3(R) spin For muons from pion decay POL(3) contains the helicity in the LAB frame when SPIN=true and SPINTRK=0.

28-Aug-2003 Steve Kahn Standardized MucGeant I/O Output File Specifications (cont.) –Also we would like the same formulism to be applicable to all of our GEANT ring simulations: TETRA RFOFO Garren-Kirk ring –We would also like to have the liberty to calculate the emittance anywhere we want. Place a virtual volume named CALC to be placed anywhere one desires to make the emittance calculations. This would be done merely by placing this volume description in the RCP data file. –The issues are the same as with the input files. We must transform from the global coordinates to the local ICOOL reference system.

28-Aug-2003 Steve Kahn Standardized MucGeant I/O More Output Specifications –In order to facilitate the transformation to ICOOL reference system the user will have to supply functions for this reference system description since they are different for TETRA, RFOFO, etc. Specifically, FUNCTION REFERENCE_LENGTH(real[3]) which gives the geometric reference arc path length from the global position of the CALC virtual volume for the first turn. The correct RING_CIRCUMFERENCE for the chosen ring should be in the RCP file. This is necessary for the turn definition and the ICOOL Z definition. Current Status: –I am currently working on the output phase to write a file for ECALC9.