JC and Marina 12/18/00 Pixel Detector Simulation with Magnetic Field  Effects with magnetic Field o Deflection o Effective mobility o Non-constant Hall.

Slides:



Advertisements
Similar presentations
Beam-plug under M2 and HCAL shielding studies Robert Paluch, Burkhard Schmidt October 9,
Advertisements

Analysis for J2 chamber Yousuke Kataoka (University of Tokyo) Atsuhiko Ochi, Yuki Edo (Kobe University) 11 / 12 / 2012 Micromegas weekly meeting 1.
Sabino Meola Charged kaon group meeting 12 October 2005 Status of analysis.
2 Introduction   MiniCal test-beam studies started at the beginning of March (till March 6 we only had 17 APD’s, then 33 APD’s)   A few days were.
May 14, 2015Pavel Řezníček, IPNP Charles University, Prague1 Tests of ATLAS strip detector modules: beam, source, G4 simulations.
Daniele De Gruttola (TOF group – Salerno University and INFN ) 2009 cosmic rays data analysis 09/Dec/09 ALICE - TOF meeting - CERN.
June 6 th, 2011 N. Cartiglia 1 “Measurement of the pp inelastic cross section using pile-up events with the CMS detector” How to use pile-up.
Study of GEM-TPC Performance in Magnetic Fields Dean Karlen, Paul Poffenberger, Gabe Rosenbaum University of Victoria and TRIUMF, Canada 2005 ALCPG Workshop.
Precision Measurement of F 2 with H1 Workshop on DIS and QCD, Florence, Max Klein for the H1 Collaboration Towards today The Measurement Results.
Standalone VeloPix Simulation Jianchun Wang 4/30/10.
Offline Code for Next Beam Test Jianchun Wang 08/06/01.
JC and Marina 12/18/00 Pixel Detector Simulation with Magnetic Field  Effects with magnetic Field o Deflection o Effective mobility o Non-constant Hall.
MC Study of B°  S Jianchun Wang Syracuse University BTeV meeting 06/27/01.
MC Study on B°  S (Status Report) Jianchun Wang Syracuse University BTeV meeting 05/25/01.
Atmospheric Neutrino Event Reconstruction Andy Blake Cambridge University June 2004.
Status on Testbeam Analysis Jianchun Wang Syracuse University VELO meeting, August 28, 2007.
Status of  b Scan Jianchun Wang Syracuse University Representing L b scanners CLEO Meeting 05/11/02.
Increasing Field Integral between Velo and TT S. Blusk Sept 02, 2009 SU Group Meeting.
Slide 1 sCVD Diamond for the CMS Pixel Detector May 2004 R.Stone, Rutgers J.Doroshenko, L.Perera, S.Schnetzer RD42 Collaboration Meeting Overview.
Jianchun Wang Marina Artuso Syracuse University 11/06/00 MC Simulation of Silicon Pixel Detector.
JC and Marina 04/02/01 Pixel Cross Talk Study  Modeling: Linear coupling between neighbor rows  Parameters in the simulation:  FPIX0-Pstop gain curve.
Effective Depletion Depth JC & Marina. 04/30/01Jianchun (JC) Wang2 Depletion Depth Methods FPIX0 pstop at 30° X inc Depth: d  XiXi.
VELO ADC vs Charge Calibration Jianchun Wang April 16, 2008 This is an update to the presentation at April 11 st VELO Group Meeting. A new scan data of.
FPIX0 Electronic Test Marina Artuso Paul Gelling Jianchun Wang  The system works fine with charge injection calibration  Gain curve, threshold, and noise.
Responsibility on Next Beam Test Jianchun Wang Syracuse University BTeV meeting 06/27/01.
MC Study on B°  J/  ° With J/      °     Jianchun Wang Syracuse University BTeV meeting 03/04/01.
Analysis work by: Marina Artuso Sheldon Stone Jianchun Wang CBX note available: /homes/cleo/sls/dompi.ps Study of B  D   Jianchun Wang 05/12/00.
Velo to T Alignment - Reminder General Strategy  Perform relative VELO-to-IT/OT alignment using  X,  Y at the center of magnet and  X,  Y (each.
Analysis work by: Rachid Ayad Sheldon Stone Jianchun Wang CBX note available: /homes/cleo/sls/ds4pi.ps Status of B  D  (4  )   analysis Jianchun.
STAR Collaboration Meeting, Nantes, July2002 SVT Analysis/Status Update Jun Takahashi – University of Sao Paulo.
M. Aleppo - A measurement of Lorentz angle of rad-hard pixel sensors - Pixel 2000 Genova 1 A measurement of Lorentz angle of rad-hard pixel sensors Dipartimento.
Karsten Büßer Beam Induced Backgrounds at TESLA for Different Mask Geometries with and w/o a 2*10 mrad Crossing Angle LCWS 2004 Paris April 19 th 2004.
Progress on BR(K L  p + p - ) using a double-tag method A. Antonelli, M. Antonelli, M. Dreucci, M. Moulson CP working group meeting, 25 Feb 2003.
2016/6/4 Taka Kondo (KEK) 1 Issues of the SCT Digitization model 2 nd meeting of SCT Digitization TF Taka Kondo (KEK) 1.Current SCT digitization.
Impact parameter resolution study for ILC detector Tomoaki Fujikawa (Tohoku university) ACFA Workshop in Taipei Nov
August 26, 2003P. Nilsson, SPD Group Meeting1 Paul Nilsson, SPD Group Meeting, August 26, 2003 Test Beam 2002 Analysis Techniques for Estimating Intrinsic.
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.
“Vertexig and tracking ” Entirely based on works and results by: S. Rossegger, R. Shahoyan, A. Mastroserio, C. Terrevoli Outline: Comparison Fast simulation.
August 26, 2003P. Nilsson, SPD Group Meeting1 Paul Nilsson, SPD Group Meeting, August 26, 2003 Test Beam 2002 Pixel Response Simulation: Update Jan Conrad.
T. Lari – INFN Milan Status of ATLAS Pixel Test beam simulation Status of the validation studies with test-beam data of the Geant4 simulation and Pixel.
Pixel Results from CRAFT09 U. Langenegger (PSI), G. Giurgiu (JHU) Pixel General Meeting November 10, 2009.
The Luminosity Calorimeter Iftach Sadeh Tel Aviv University Desy ( On behalf of the FCAL collaboration ) June 11 th 2008.
Study of Belle Silicon Vertex Detector Intrinsic Resolution Saša Fratina, Jožef Stefan Institute, Ljubljana, Slovenia for Belle SVD group.
DN/d  and dN/dp T analysis status Gabor Veres for the working group QCD meeting, Jan 12, 2010.
Update on Diffractive Dijets Hardeep Bansil University of Birmingham 12/07/2013.
A. SarratILC TPC meeting, DESY, 15/02/06 Simulation Of a TPC For T2K Near Detector Using Geant 4 Antony Sarrat CEA Saclay, Dapnia.
July 24,2000Gabriele Chiodini1 Measurements in magnetic field - digression Lorentz angle measurements –ATLAS measurements – CMS measurements Radiation.
10/25/2007Nick Sinev, ALCPG07, FNAL, October Simulation of charge collection in chronopixel device Nick Sinev, University of Oregon.
BTeV Beam Test Results Jianchun Wang Syracuse University Representing J.A. Appel, J.N. Butler, G. Cardoso, H. Cheung, G. Chiodini, D.C. Christian, E.E.
Mitglied der Helmholtz-Gemeinschaft Hit Reconstruction for the Luminosity Monitor March 3 rd 2009 | T. Randriamalala, J. Ritman and T. Stockmanns.
L. Bosisio - SVT TDR Meeting SuperB SVT Update on Strip Parameters and Layer 3 Readout Options Irina Rashevskaya, Lorenzo Vitale, Livio Lanceri,
Pixel Offline Status Jianchun Wang Syracuse University 10/28/04, Pixel testbeam meeting.
IPHC, Strasbourg / GSI, Darmstadt
Michele Faucci Giannelli
M. Sullivan Apr 27, 2017 MDI meeting
gamma ray polarisation measurement
Design and Characterization of a Novel, Radiation-Resistant Active Pixel Sensor in a Standard 0.25 m CMOS Technology P.P. Allport, G. Casse, A. Evans,
STT pattern recognition improvements since last December meeting and
FDIRC MC Studies: PMT Coupling Options
Neutrinos from BBfit J. Brunner.
Integration and alignment of ATLAS SCT
HARPO Analysis.
HPS Collaboration meeting, JLAB, Nov 16, 2016
DE/dx Study at CEPC TPC An Fenfen
Monte Carlo simulation of the DIRC prototype
Design of active-target TPC
Imperial laser system and analysis
Gel Electrophoresis -samples with ligated DNA are loaded in a “gel” where they are run; an electric field is set up within the box -DNA has a slight charge,
LC Calorimeter Testbeam Requirements
Presentation transcript:

JC and Marina 12/18/00 Pixel Detector Simulation with Magnetic Field  Effects with magnetic Field o Deflection o Effective mobility o Non-constant Hall mobility  Comparison with magnet run

Jianchun (JC) WangSyracuse University2 Magnetic Field

Jianchun (JC) WangSyracuse University3 Deflection in Magnetic Field n+n+ n p+p+ -V 0 V  e e e e e e e e e e e e e B y  Effect of magnetic field  Effect of incident angle

Jianchun (JC) WangSyracuse University4 Deflection in Magnetic Field Assumption:  H = constant  eff =  The charge distributions are the same with B or 

Jianchun (JC) WangSyracuse University5 Effective Mobility Very small effect: B field  Cloud drifts slower  Larger Spread

Jianchun (JC) WangSyracuse University6 E-dependent Mobility Larger E  Smaller  Hall   Smaller deflection P + side larger E N+ Side Smaller E

Jianchun (JC) WangSyracuse University7 Effect of Magnetic Field With non-constant  Hall (E), and  eff The charge distributions are slightly different

Jianchun (JC) WangSyracuse University8 Conclusion We Don’t expect the magnetic field will reduce the ratio between two-pixel clusters and one-pixel clusters

Jianchun (JC) WangSyracuse University9 Magnet Run  Track at 1.3  angle ( ~ Tesla )  Measurement: R min =  Simulation ( Q th = 2.5Ke ): R min = What is wrong ?

Jianchun (JC) WangSyracuse University10 Magnet Run  Track at 1.32  ( 23 mrad ) ( ~ Tesla )  Measurement: R min =  Simulation ( Q th = 4.0Ke ): R min = Just to Play around But there is no other evidence that threshold was wrong

Jianchun (JC) WangSyracuse University11 Magnetic Field Measured with Gauss meter: 45A  Tesla Assume overall scale of the magnetic field uncertain Use MC simulation to fit  Tesla (error?) Error of Hall factor (  Hall /  =1.15) can make up the difference

Jianchun (JC) WangSyracuse University12 Summary  MC simulation accurate both for drift and B field simulation  Magnet Run data is not fully understood yet