Transition Radiation Simulations

Slides:

Advertisements

Similar presentations

METO 621 Lesson 6. Absorption by gaseous species Particles in the atmosphere are absorbers of radiation. Absorption is inherently a quantum process. A.

Advertisements

Geant4 simulation of roman pots A. Kupco, P. Ruzicka, M. Tasevsky.

GEANT 4 simulation of energy deposited in KASCADE-Grande detectors Carpathian Summer School of Physics 2012.

Hadronic and Electromagnetic Physics: special applications V.Ivanchenko BINP, Novosibirsk, Russia & CERN, Geneve, Switzerland.

MARS flux simulations - update Sergei Striganov Fermilab August 12, 2009.

28 April 2005Ckov1 Update -- S. Kahn1 Update to the Upstream Cherenkov  -  Separation Steve Kahn Brookhaven National Lab May 2, 2005 Detector Tele-Meeting.

Tracker Reconstruction SoftwarePerformance Review, Oct 16, 2002 Summary of Core “Performance Review” for TkrRecon How do we know the Tracking is working?

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.

NEUTRON OPTICS & SHIELDING GROUP NATALIIA CHERKASHYNA TAP MEETING 23 RD OF JANUARY, 2014 Latest Developments on Shielding and Backgrounds.

DESY: From High Energy Physics to Synchrotron Radiation Accelerator Operation in a changing Environment Michael Bieler DESY: From High Energy Physics to.

Quest for omega mesons by their radiative decay mode in √s=200 GeV A+A collisions at RHIC-PHENIX ~Why is it “Quest”?~ Simulation Study Real Data Analysis.

Calorimeters Chapter 4 Chapter 4 Electromagnetic Showers.

RICH SIMULATION USING GEANT4 S.EASO, RAL OBJECTIVES OF THE SIMULATION. CURRENT STATUS AND PLANS. INTEGRATION WITH LHCb SOFTWARE. SUMMARY.

21 Jun 2010Paul Dauncey1 First look at FNAL tracking chamber alignment Paul Dauncey, with lots of help from Daniel and Angela.

VICOMTECH VISIT AT CERN CERN 2013, October 3 rd & 4 th O.COUET CERN/PH/SFT DATA VISUALIZATION IN HIGH ENERGY PHYSICS THE ROOT SYSTEM.

Difference between Roman Pots and VELO Very forward tracking is typically done using detectors located in Roman pots. They are far away from the interaction.

Measurement of Vus. Recent NA48 results on semileptonic and rare Kaon decays Leandar Litov, CERN On behalf of the NA48 Collaboration.

WEEK 1 You have 10 seconds to name…

Calorimetry for Deeply Virtual Compton Scattering in Hall A Alexandre Camsonne Hall A Jefferson Laboratory Workshop on General Purpose High Resolution.

Physics Data Libraries: Content and Algorithms for Improved Monte Carlo Simulation Physics data libraries play an important role in Monte Carlo simulation:

26 Jan 2010Paul Dauncey1 TPAC papers Paul Dauncey.

HIGH GRANULARITY CALORIMETER ANALYSIS SARAH MARIE BRUNO CMS - CALTECH GROUP SUPERVISORS: ADOLF BORNHEIM, LINDSEY GRAY, MARIA SPIROPULU.

J.Feltesse1 Measurement of F L the longitudinal structure function at HERA Low x meeting, Lisbon, Portugal 28 June 2006.

1 Fast Pixel Simulation Howard Wieman, Xiangming Sun Lawrence Berkeley Lab.

Study of SoLID Baffle, Background and Trigger Zhiwen Zhao UVa, ODU&JLab 2014/07/09 1.

2/26/2014PHY 770 Spring Lecture 131 PHY Statistical Mechanics 12:00 * -1:45 PM TR Olin 107 Instructor: Natalie Holzwarth (Olin 300) Course.

Zeldovich-90, Prethermalization in early Universe D. Podolsky, G. Felder, L. Kofman, M. Peloso CITA (Toronto), Landau ITP (Moscow), University.

SoLID Background Update Zhiwen Zhao UVa 2013/11/08 1.

GUINEA-PIG: Beam-beam interaction simulation status M. Alabau, P. Bambade, O. Dadoun, G. Le Meur, C. Rimbault, F. Touze LAL - Orsay D. Schulte CERN - Genève.

Feb. 3, 2007IFC meeting1 Beam test report Ph. Bruel on behalf of the beam test working group Gamma-ray Large Area Space Telescope.

First collisions in LHC

Compact Linear Collider

Thermal Energy & Heat.

RADIATIVE CORRECTIONS TO IN PANDAROOT

What’s an X-Ray Ionization.

Ian Bird WLCG Workshop San Francisco, 8th October 2016

M. Brigida, F. de Palma, C. Favuzzi, P. Fusco, F. Gargano, N

Forward Tagger Simulations

Energy deposition studies on magnets. Aim. First applications

Panagiotis Kokkas Univ. of Ioannina

Detection of muons at 150 GeV/c with a CMS Preshower Prototype

of secondary light ion beams

of secondary light ion beams

CS 591 S1 – Computational Audio -- Spring, 2017

Cell simulation in Geant4 Phase 1

Detector Configuration for Simulation (i)

Online Gifts Buy for wishes happy mother's day to yours choice and with happy gifts find here:

Grid Canada Testbed using HEP applications

Waves, Electromagnetic Spectrum & Color Theory

Correction of saturation effect of ICCD

Status of ATLAS and CMS and prospects for the run

10 ways to cheat with energy

مديريت موثر جلسات Running a Meeting that Works

Multi-Turn Extraction for PS2 Preliminary considerations

P.E Survey Questions Yes No 7% % Do you enjoy P.E? % 0%

Daily Homework Sheet Monday Tuesday Wednesday Thursday Friday

Warm-Up What and 3 sources of error in the flame test lab? (Don’t just say “we messed up.” Consider how you could have done things better or how the.

Classifying Matter and

Lesson Quizzes Standard Lesson Quiz

33 Unit 1:2 Human Organ Systems The Digestive System

33 Unit 1:2 Human Organ Systems The Digestive System

Spellings – sentences and dictionary definitions.

PHY Statistical Mechanics 12:00* -1:45 PM TR Olin 107

The new ATLAS Fast Calorimeter Simulation

Extended Registration KS3

Presentation transcript:

Transition Radiation Simulations Natalie Zimmer

Transition Radiation Only known way to distinguish between p, π, & k’s at extremely high energies p & k separation not good enough- currently about 1 in 10-2 p misidentified as k Need to improve by a factor of 100

CERN Experiment Very-forward direction experiment under way Need TR to identify secondary particles Have 8m to optimize photon production

GEANT4 Simulations So far have only been done on a very small scale Ideal simulations could take days to weeks to run HPC allows for reasonable runtimes