Technical Forum 1 New Requests & Requirements Geant4 Technical Forum Mar 2005 Editor J. Apostolakis.

Slides:



Advertisements
Similar presentations
EvtGen in ATLAS/LHC Roger W.L. Jones James R. Catmore Maria Smizanska Lancaster University, UK.
Advertisements

Page 1/28 Mar 2008 SGE A Monte-Carlo Simulation of the Stern-Gerlach Experiment Dr. Ahmet BİNGÜL Gaziantep Üniversitesi Fizik Mühendisliği Bölümü Nisan.
Adding electronic noise and pedestals to the CALICE simulation LCWS 19 – 23 rd April Catherine Fry (working with D Bowerman) Imperial College London.
Physics of fusion power Lecture 6: Conserved quantities / Mirror device / tokamak.
Jörgen Sjölin Stockholm University LHC experimental sensitivity to CP violating gtt couplings November, 2002 Page 1 Why CP in gtt? Standard model contribution.
X-Ray Propagation Simulation Student: Jing Yee Chee Advisors: Kenneth D. Finkelstein David Sagan Georg H. Hoffstaetter 6/17/20151.
Physics of fusion power Lecture 8: Conserved quantities / mirror / tokamak.
14 User Documents and Examples I SLAC Geant4 Tutorial 3 November 2009 Dennis Wright Geant4 V9.2.p02.
Highlights of latest developments ESA/ESTEC Makoto Asai (SLAC)
Development of an Interface for Using EGS4 Physics Processes in Geant4 K.Murakami (KEK) 27/Mar./
LHC  Facts and figures  Experiments involved  Aims  How it works.
Jianchun Wang Marina Artuso Syracuse University 11/06/00 MC Simulation of Silicon Pixel Detector.
LHC’s Second Run Hyunseok Lee 1. 2 ■ Discovery of the Higgs particle.
Summary of Work Zhang Qiwei INFN - CIAE. Validation of Geant4 EM physics for gamma rays against the SANDIA, EPDL97 and NIST databases.
User Documents and Examples I Sébastien Incerti Slides thanks to Dennis Wrigth, SLAC.
Incoherent pair background processes with full polarizations at the ILC Anthony Hartin JAI, Oxford University Physics, Denys Wilkinson Building, Keble.
Implementing a dual readout calorimeter in SLIC and testing Geant4 Physics Hans Wenzel Fermilab Friday, 2 nd October 2009 ALCPG 2009.
Magnetic Forces and Torques
Goal: To understand Electro- magnetic fields Objectives: 1)To learn about Magnetic Fields 2)To be able to calculate the magnitude of Magnetic Forces 3)To.
Computational Model of Energetic Particle Fluxes in the Magnetosphere Computer Systems Yu (Evans) Xiang Mentor: Dr. John Guillory, George Mason.
Pavel Šťavina, Bratislava 2004 Slovak contribution to experiment ATLAS  Even though Slovakia is small country with limited finances we have fulfilled.
Radius To use a Compton polarimeter, the possible range of the backscattered photons’ energy should be calculated. Applying the laws of conservation of.
Computing Performance Recommendations #13, #14. Recommendation #13 (1/3) We recommend providing a simple mechanism for users to turn off “irrelevant”
We report the result of a beam test on a prototype of Astronomical hard X-ray/soft gamma-ray Polarimeter, PoGO (Polarized Gamma-ray Observer). PoGO is.
Resonant magnetic x-ray scattering and Summary Resonant scattering –Why do it? –What is it? –How is it done? –Example(s) The Real World …. CaFe 2 As 2.
G4MICE Status and Plans 1M.Ellis - CM24 - RAL - 31st May 2009  Firstly, a correction to the agenda:  I failed to spot a mistake in the agenda that I.
Simulation of the energy response of  rays in CsI crystal arrays Thomas ZERGUERRAS EXL-R3B Collaboration Meeting, Orsay (France), 02/02/ /03/2006.
FLUKA dose and fluence simulations for CBM experiment I.Kadenko, O.Bezshyyko, V.Pluyko, V.Shevchenko National Taras Shevchenko University of Kiev.
Detector Simulation Presentation # 3 Nafisa Tasneem CHEP,KNU  How to do HEP experiment  What is detector simulation?
Update Chris Rogers, Analysis PC, 13/07/06. State of the “Accelerator” Simulation Field model now fully implemented in revised MICE scheme Sanity checking.
New software library of geometrical primitives for modelling of solids used in Monte Carlo detector simulations Marek Gayer, John Apostolakis, Gabriele.
LHCb production experience with Geant4 LCG Applications Area Meeting October F.Ranjard/ CERN.
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.
Introduction What is detector simulation? A detector simulation program must provide the possibility of describing accurately an experimental setup (both.
Two photon physics with forward detectors Beata Krupa, Leszek Zawiejski Institute of Nuclear Physics Polish Academy of Sciences 22nd FCAL Collaboration.
1 Background radiation studies in LHCb with GAUSS/Geant4 Giuseppe G. Daquino PH/SFT.
PIXEL Slow Simulation Xin Li 3/16/2008. CMOS Active Pixel Sensor (APS) Epitaxy is a kind of interface between a thin film and a substrate. The term epitaxy.
Geant4 CPU performance : an update Geant4 Technical Forum, CERN, 07 November 2007 J.Apostolakis, G.Cooperman, G.Cosmo, V.Ivanchenko, I.Mclaren, T.Nikitina,
RICH Simulation in LHCb LHC Detector Simulation Workshop S.Easo, RAL, On behalf of LHCb–RICH group.
Geant4 release 5.1 summary Gabriele Cosmo EP/SFT.
Geant4 is a toolkit to simulate the passage of particles through matter, and is widely used in HEP, in medical physics and for space applications. Ongoing.
Maria Grazia Pia, INFN Genova and CERN1 Geant4 highlights of relevance for medical physics applications Maria Grazia Pia INFN Genova and CERN.
7.2 Magnetic Field Strength p. 274 Calculating Magnetic Field Strength A moving charged particle that enters a magnetic field at any direction other than.
PoGO_G4_ ppt1 Study of optimized fast scintillator length for the astronomical hard X- ray/soft gamma-ray polarimeter PoGO November 1, 2004 Tsunefumi.
1 Giuseppe G. Daquino 26 th January 2005 SoFTware Development for Experiments Group Physics Department, CERN Background radiation studies using Geant4.
Updates on requirements from previous TF meetings Geant4 Technical Forum January 31 st, 2007 J. Apostolakis, M. Asai (SLAC) on behalf of Geant4 collaboration.
ArgonneResult_ ppt1 Comparison of data and simulation of Argonne Beam Test July 10, 2004 Tsunefumi Mizuno
ArgonneResult_ ppt1 Results of PoGO Argonne Beam Test PoGO Collaboration meeting at SLAC, February 7, 2004 Tsunefumi Mizuno
O Tsunefumi Mizuno, Tuneyoshi Kamae, Jonny Ng, Hiroyasu Tajima (SLAC), John W. Mitchell, Robert Streitmatter (NASA GSFC), Richard C. Fernholz, Edward Groth.
A Short Course on Geant4 Simulation Toolkit Introduction
Alex Howard, Imperial College Slide 1 July 2 nd 2001 Underground Project UNDERGROUND PROJECT – Overview and Goals Alex Howard Imperial College, London.
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.
Monthly video-conference, 18/12/2003 P.Hristov1 Preparation for physics data challenge'04 P.Hristov Alice monthly off-line video-conference December 18,
Jiaxin Wang and Robin P. Gardner Oct 6 th 2011, CEAR at NC State University, Raleigh, NC.
Updates on requirements from previous TF meetings
UNIT IV Molecules.
EvtGen Miniworkshop, Patrick Robbe LAL Orsay, 21 Jan 2005
Patrick Robbe, LAL Orsay, 13 May 2004
June 1, 2004 Tsunefumi Mizuno Expected Modulation Factor of PoGO calculated with Geant4 Simulator with PoGO-fix June 1, 2004 Tsunefumi.
Progress with Spin Tracking in GEANT4
Analysis of 14/20 mrad Extraction Line Energy Chicane
User Documents and Examples I
CMS requirements for G4 TF on
Related OSE's.
GEANT Simulations and Track Reconstruction
Status of energy deposition studies IR7
Background issues for the Super-B background simulation team
Marc Verderi GEANT4 collaboration meeting 01/10/2002
Projects by User Groups in Spain: Application to g-ray Spectrometry
J.J Thomson.
Presentation transcript:

Technical Forum 1 New Requests & Requirements Geant4 Technical Forum Mar 2005 Editor J. Apostolakis

Technical Forum 2 1. Polarised Rayleigh scattering Originator : PoGO (Tsunefumi Mizuno) The astronomical hard X-ray polarimeter called PoGO, aims to measure the polarization from astrophysical object in keV range by measuring the asymmetry in azimuthal scattering angle. We discovered that the Rayleigh scattering process in Geant4 does not deal with the photon polarization, and consequently gave an artificially small modulation. Since the Rayleigh scattering cross-section is not negligible in the energy of our interest, this needs to be solved to simulate accurately. Request to implement the polarization process in Rayleigh Scattering –Offer to provide code we created as sample if needed. Since the energy bands of astrophysical Compton polarimeters are similar with each other, the implementation of polarized Rayleigh scattering is expected to be valuable to the community.

Technical Forum 3 2. Selective verbosity Originator: LHCb (G. Corti) We would like more configurable debugging features. –It is possible to follow in details various aspects of the simulation by setting verbose levels. –This is very hard to use when tracking complete pp events because millions of G4Track are produced. It would be very useful to be able to selectively turn on such verbose for a single G4Track, a single region of the detector, a combination of the two.

Technical Forum 4 3. Treat particles with dipole moments Originator: AD ( Bertalan Juhasz ) The user should be able to calculate the force acting on the magnetic (and possibly electric) dipole moment of a (neutral or charged) particle in an inhomogeneous magnetic (electric) field [F = mu * grad B] –for this, the magnetic dipole moment of a particle should be available for the equation of motion; Note that the magnetic moment is not necessarily a vector of constant magnitude, as its magnitude and direction might depend on e.g. the magnitude and direction of the external magnetic field Potentially no new standard G4 equation of motion class is needed; the force should be calculated by a user-derived equation of motion class

Technical Forum 5 4. Neutron data for additional elements Originators: (BaBar, Vanderbilt) BaBar needs the elements Nd (Neodymium) and Sm (Samarium) added to the high precision neutron models. In addition Vanderbilt are asking that As, In, Ge, Ga, Sb, Hg, Cd, Te, and Gd also be added. Seconded by ESA.

Technical Forum 6 New proposed ‘platforms’: gcc Originator: ATLAS (D. Quarrie, A. Nairz) ATLAS, and the other LCH experiments, intend for the next two supported platforms to be: –gcc with SLC3 in 32-bit mode (IA32) –gcc with SLC3 in 64-bit mode (AMD64) Current understanding (which should be checked) is that these will be binary compatible with both Intel & AMD 32-platforms and EM64T Intel 64-bit platforms (not IA64 - Itanium). The [requested] timescale is that porting of external software to IA32 is about to start [now] and we hope to have a prototype ATLAS port available in Sept, but not yet in production. Also interested to maintain compatibility with CLHEP 1.8 for approximately the next 3 months.

Technical Forum 7 Other A) Example for new particles Originator : Atlas/CMS Example for creating new type of particles: creating a new particle and a modified primary transformer that creates tracks Use case: creating new heavy sleptons particles, to investigate potential new physics in LHC experiment detectors. B) Python UI Originator : ATLAS (A. Dell’Acqua, A. Nairz) More support for a python UI in G4 (not only the current UI/macro version). C) User Limits per region Originator : EXO experiment (SLAC) Enable choice of User Limits per region "Given Geant4 allows defining cuts per region, why it does not allow defining G4UserLimits to a region?“ Notes: A first examination showed that this will not conflict with existing use cases for User Limits.