Extra Energy in Inelastic Hadronic Interactions in GHEISHA / GEANT4

Slides:



Advertisements
Similar presentations
Stefan Roesler SC-RP/CERN on behalf of the CERN-SLAC RP Collaboration
Advertisements

ESTIMATING THE FAKE LEPTON BACKGROUND IN A SEARCH FOR PAIR PRODUCED STOPS AT CMS David Kolchmeyer Advisor: Alberto Graziano.
Calorimetry and Showers Learning Objectives Understand the basic operation of a calorimeter (Measure the energy of a particle, and in the process, destroy.
TIME-LIKE BARYON FORM FACTORS: EXPERIMENTAL SITUATION AND POSSIBILITIES FOR PEP-N Roberto Calabrese Dipartimento di Fisica and I.N.F.N. Ferrara, Italy.
Energy and momentum: Collisions and conservation laws.
Final state study Jaewon Park University of Rochester MINERvA/Jupiter Group Meeting, May 09, 2007.
Physics list update Phone conference 18/2 -04 Rikard Sandström Geneva University.
Angular Distribution of Gamma-rays from Up-to-date p-p Interactions GLAST Science Lunch Talk Aug 3, 2006 Niklas Karlsson SLAC / KTH
The Particle Zoo. Too Many Particles Far from just finding Protons Neutrons Electrons Neutrinos and their antiparticles, during the 20 th century many.
Dec 2000 GEANT4 Workshop - David Bailey Hadronic Interactions 1 Checking Basic Characteristics of Hadronic Shower Parameterizations in GHEISHA / GEANT4.
My Chapter 30 Lecture.
Hadronic Models Problems, Progress and Plans Gunter Folger Geant4 Workshop, Lisbon 2006.
Periodic Table Basics. Finding the number of Atomic Particles # of protons = to the atomic # # of electrons = to the atomic # To determine the # of neutrons.
Extending the Bertini Cascade Model to Kaons Dennis H. Wright (SLAC) Monte Carlo April 2005.
Event generator comparison Zhiwen Zhao 2013/12/03 original 2014/02/12 update 2014/11/04 update.
Kinematics of  + n   p   0  p reaction Susumu Oda 2007/04/10-19.
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 30: Particle Physics Fundamental.
Status of particle_hp Pedro Arce Emilio Mendoza Daniel Cano-Ott (CIEMAT, Madrid)
W JamboreeEric Lançon - ALEPH Week - January Jetset vs Herwig … Once more III Jetset vs Herwig on same selected events.
Introduction The statistical model approach is established by analysis of particle ratios of the high energy heavy ion collisions in GSI-SIS to CERN-SPS.
Particle Production of Carbon Target with 20Tto2T5m Configuration at 6.75 GeV (Updated) X. Ding, UCLA Target Studies April 3, /3/14.
DISCOVERY OF THE NEUTRON
The Geant3 tale ➢ Motivation... ➢ Why AliROOT+G3 are not reproducing any more the measurements ? ➢ Why stand alone code do reproduce measurements ? talk.
Neutron measurement with nuclear emulsion Mitsu KIMURA 27th Feb 2013.
J-PARC でのハイパー核ガンマ線分光実験用 散乱粒子磁気スペクトロメータ検出器の準備 状況 東北大理, 岐阜大教 A, KEK B 白鳥昂太郎, 田村裕和, 鵜養美冬 A, 石元茂 B, 大谷友和, 小池武志, 佐藤美沙子, 千賀信幸, 細見健二, 馬越, 三輪浩司, 山本剛史, 他 Hyperball-J.
Summary of hadronic tests and benchmarks in ALICE Isidro González CERN EP-AIP/Houston Univ. Geant4 workshop Oct
P460 - Relativity21 Lorentz Transformations (px,py,px,E) are components of a 4-vector which has same Lorentz transformation px’ =  (px + uE/c 2 ) u =
Search for High-Mass Resonances in e + e - Jia Liu Madelyne Greene, Lana Muniz, Jane Nachtman Goal for the summer Searching for new particle Z’ --- a massive.
1 Hadronic calorimeter simulation S.Itoh, T.Takeshita ( Shinshu Univ.) GLC calorimeter group Contents - Comparison between Scintillator and Gas - Digital.
The Particle Zoo Particle Physics Lesson 6. What are the charges? γ (photon) γ (photon) p (proton) p (proton) n (neutron) n (neutron) ν (neutrino) ν (neutrino)
An interface between HIJING & Geant4-9.5 Umm Al-Qura University-Saudi Arabia Benha University-Egypt Khaled Abdel-Waged.
Relativistic Mechanics Momentum and energy. Momentum p =  mv Momentum is conserved in all interactions.
Tau31 Tracking Efficiency at BaBar Ian Nugent UNIVERSITY OF VICTORIA Sept 2005 Outline Introduction  Decays Efficiency Charge Asymmetry Pt Dependence.
Extrapolation Techniques  Four different techniques have been used to extrapolate near detector data to the far detector to predict the neutrino energy.
Relativistic Momentum p  mu/[(1 – (u/c) 2 ] 1/2 =  mu   1     
High Energy Particle Physics
IBD Detection Efficiencies and Uncertainties
Mass of constituent parts of the nucleus:
12th Geant4 Space Users Workshop
Scattering Reactions Scattering reactions - the incident particle collides with the target nucleus Elastic scattering – a collision between a particle.
M11/TZ2/B1 B1. This question is in two parts. Part 1 is about simple harmonic motion (SHM) and a wave in a string. Part 2 is about the unified atomic mass.
Muons from the decay of charmed baryons/antibaryons
P0D reconstruction/analysis update
MINERVA Z Mass Exercise
Special Theory of Relativity
V. Uzhinsky, A Galoyan (JINR, Dubna, Russia), 2015
Hadron-structure studies at a neutrino factory
Summary of hadronic tests and benchmarks in ALICE
Detector Configuration for Simulation (i)
String Parton Models in Geant4
Highlights in Low Energy Hadronic Physics
Advanced Topics Nuclear Physics ElementaryParticles General Relativity
General Physics (PHY 2140) Lecture 37 Modern Physics Nuclear Physics
General Physics (PHY 2140) Lecture 37 Modern Physics Nuclear Physics
Main ingredient of the Fritiof model Fritiof model in Geant4
Particle physics.
General Physics (PHY 2140) Lecture 37 Modern Physics Nuclear Physics
Comparison between Geant4, Fluka and the TileCal test-beam data
Isotopes.
Relativistic Momentum
Summary of dE/dx studies in silicon and MS in muon system
Atomic Structure Lab Activity
Introducing the “Particle Players”
GEANT4: Patch-02 to Release 8.1 (released on November 10th, 2006)
NKS2 Meeting with Bydzovsky NKS2 Experiment / Analysis Status
Nuclear Reactions.
Hough-D(mc)- ππJpsi(Data)
Isotopes.
Search for X - - Pentaquark in COMPASS
Problems in π0 Reconstruction
Presentation transcript:

Extra Energy in Inelastic Hadronic Interactions in GHEISHA / GEANT4 David Bailey University of Toronto Intend to look hadronic interactions in FCAL, … But first checked basic characteristics of hadronic interactions in MC ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Extra Energy in GHEISHA - David Bailey Basic Parameters GEANT 4.2.0 ref 2 PhysicsList copied from example N02 GEANT 3.21 Particles generated at centre of huge uniform cubes side half-length = 105 km material either Liquid Hydrogen or Iron “Total Energy” is the sum of step energy losses neutrino energies ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Extra Energy in GHEISHA - David Bailey 100 GeV/c2 + in Iron ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Total Energy for 100 GeV/c2 + in hydrogen ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Total Energy for 1 GeV/c2 neutrons in hydrogen ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Sample GEANT4 1 GeV/c2 proton in Hydrogen event printout ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Kinetic Energies of some GEANT4 interactions proton 985 MeV 0 MeV proton (438 MeV) pi0 (456 MeV) neutron (248 MeV) pi+ (503 MeV) ∆Q=936MeV neutron 543 MeV proton 0 MeV proton (389 MeV) pi0 (297 MeV) neutron (543 MeV) ∆Q=821MeV ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Extra Energy in GHEISHA - David Bailey Gheisha Fortran Gheisha seems to calculate the target particle mass by counting the number of outgoing baryons. SUBROUTINE TWOCLU(IPPP,NFL,AVERN) / SUBROUTINE GENXPT(IPPP,NFL,AVERN) C *** GENERATION OF X- AND PT- VALUES FOR ALL PRODUCED PARTICLES *** C *** NVE 01-AUG-1988 CERN GENEVA *** … C** LORENTZ TRANSFORMATION IN LAB SYSTEM C** 27 TARG=0. DO 36 I=1,NT IF(PV(5,I).GT.0.5) TARG=TARG+1. CALL LOR(I,MX2,I) 36 CONTINUE C*DCB --> David Bailey modification to prevent counting C*DCB incoming baryon as a target particle if (amas.gt.0.5) targ=targ-1. ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

1 GeV/c2 neutron in hydrogen, Total Energy ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Total Energy of 100 GeV/c2 pi+ in Iron ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Extra Energy in GHEISHA - David Bailey GEANT 4 has similar code same place as fix to previous energy non-conservation bug // $Id: G4HEInelastic.cc,v 1.5 2000/07/09 09:48:35 hpw Exp $ … // Lorentz transformation in lab system targ = 0; for( i=0; i < vecLen; i++ ) { if( pv[i].getType() == baryonType )targ++; if(verboseLevel > 1) pv[i].Print(i); pv[i].Lor( pv[i], pvmx[1] ); } if ( targ <1) targ = 1; (Twice) but my first attempt (yesterday) to “fix” it failed, and I noticed something else … ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Total Energy for 1 GeV/c2 antineutrons in hydrogen ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey

Extra Energy in GHEISHA - David Bailey Summary GHEISHA inelastic hadronic interactions have some “peculiarities”. These are old enough that they must be considered GEANT3 “features”. GEANT4 accurately reproduces these “features”. Do we want these “features” in GEANT4? ATLAS GEANT4 - 6 November 2000 Extra Energy in GHEISHA - David Bailey