4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 1 New ideas and old doubts about the calorimeter shaking procedure Andrea Venturi INFN.

Slides:



Advertisements
Similar presentations
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Advertisements

LC Calorimeter Testbeam Requirements Sufficient data for Energy Flow algorithm development Provide data for calorimeter tracking algorithms  Help setting.
Lauri A. Wendland: Hadronic tau jet reconstruction with particle flow algorithm at CMS, cHarged08, Hadronic tau jet reconstruction with particle.
CMS reconstruction and identification Part II CMS reconstruction and identification Part II A. Nikitenko Tau jetsTau jets Missing E T (briefly)Missing.
P. Gay Energy flow session1 Analytic Energy Flow F. Chandez P. Gay S. Monteil CALICE Coll.
Energy Flow in CMS ;-P 1 Colin Bernet & Patrick Janot, for the CMS PF group. PF discussion, Feb 15, 2011.
22/5/2011 Particle-ID and Tracking performance in CLIC_ILD1/27 CLIC_ILD particle identification and tracking performance J. Nardulli This talk in 2 parts:
Testbeam Requirements for LC Calorimetry S. R. Magill for the Calorimetry Working Group Physics/Detector Goals for LC Calorimetry E-flow implications for.
Ties Behnke, Vasiliy Morgunov 1SLAC simulation workshop, May 2003 Pflow in SNARK: the next steps Ties Behnke, SLAC and DESY; Vassilly Morgunov, DESY and.
PFA on SiDaug05_np Lei Xia ANL-HEP. PFA outline Calibration of calorimeter –Done –Not tuned for clustering algorithm Clustering algorithm –Done: hit density.
Some early attempts at PFA Dhiman Chakraborty. LCWS05 Some early attempts at PFA Dhiman Chakraborty2 Introduction Primarily interested in exploring the.
Bob Jacobsen July 22, 2003 From Raw Data to Physics From Raw Data to Physics: Reconstruction and Analysis Introduction Sample Analysis A Model Basic Features.
 Track-First E-flow Algorithm  Analog vs. Digital Energy Resolution for Neutral Hadrons  Towards Track/Cal hit matching  Photon Finding  Plans E-flow.
 Performance Goals -> Motivation  Analog/Digital Comparisons  E-flow Algorithm Development  Readout R&D  Summary Optimization of the Hadron Calorimeter.
Sept 30 th 2004Iacopo Vivarelli – INFN Pisa FTK meeting Z  bb measurement in ATLAS Iacopo Vivarelli, Alberto Annovi Scuola Normale Superiore,University.
Clustering: Algorithm development and analysis R. Cassell, G. Bower.
LPC Jet/Met meeting 1/12/2006L. Perera1 Jet/Calorimeter Cluster Energy Corrections – Status Goal: To improve the individual jet energy determination based.
1 Hadronic In-Situ Calibration of the ATLAS Detector N. Davidson The University of Melbourne.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
Tau Jet Identification in Charged Higgs Search Monoranjan Guchait TIFR, Mumbai India-CMS collaboration meeting th March,2009 University of Delhi.
Progress with the Development of Energy Flow Algorithms at Argonne José Repond for Steve Kuhlmann and Steve Magill Argonne National Laboratory Linear Collider.
Preliminary comparison of ATLAS Combined test-beam data with G4: pions in calorimetric system Andrea Dotti, Per Johansson Physics Validation of LHC Simulation.
Optimizing DHCAL single particle energy resolution Lei Xia 1 CALICE Meeting LAPP, Annecy, France September 9 – 11, 2013.
Introduction Multi-jets final states are of major interest for the LC Physics EFlow : An essential test to design the foreseen detector Software (Algorithms)
Summary of PHOS Internal Notes (part I) Rafael Diaz Valdes 10/25/20151.
Studies of the jet fragmentation in p+p collisions in STAR Elena Bruna Yale University STAR Collaboration meeting, June
W JamboreeEric Lançon - ALEPH Week - January Jetset vs Herwig … Once more III Jetset vs Herwig on same selected events.
Event Reconstruction in SiD02 with a Dual Readout Calorimeter Detector Geometry EM Calibration Cerenkov/Scintillator Correction Jet Reconstruction Performance.
25 sep Reconstruction and Identification of Hadronic Decays of Taus using the CMS Detector Michele Pioppi – CERN On behalf.
May 1-3, LHC 2003V. Daniel Elvira1 CMS: Hadronic Calorimetry & Jet/ Performance V. Daniel Elvira Fermilab.
Feb. 7, 2007First GLAST symposium1 Measuring the PSF and the energy resolution with the GLAST-LAT Calibration Unit Ph. Bruel on behalf of the beam test.
Pandora calorimetry and leakage correction Peter Speckmayer 2010/09/011Peter Speckmayer, WG2 meeting.
7 December SLHC Calo Trigger Simulation Status Report Kevin Flood, Michail Bachtis University of Wisconsin, Madison.
Positional and Angular Resolution of the CALICE Pre-Prototype ECAL Hakan Yilmaz.
CBM ECAL simulation status Prokudin Mikhail ITEP.
Taikan Suehara, ILC-Asia physics meeting, 2009/06/13 page 1 Tau-pair analysis for LoI+ Taikan Suehara ICEPP, The Univ. of Tokyo.
PHOTON RECONSTRUCTION IN CMS APPLICATION TO H   PHOTON RECONSTRUCTION IN CMS APPLICATION TO H   Elizabeth Locci SPP/DAPNIA, Saclay, France Prague.
PFAs – A Critical Look Where Does (my) SiD PFA go Wrong? S. R. Magill ANL ALCPG 10/04/07.
Bangalore, India1 Performance of GLD Detector Bangalore March 9 th -13 th, 2006 T.Yoshioka (ICEPP) on behalf of the.
13 July 2005 ACFA8 Gamma Finding procedure for Realistic PFA T.Fujikawa(Tohoku Univ.), M-C. Chang(Tohoku Univ.), K.Fujii(KEK), A.Miyamoto(KEK), S.Yamashita(ICEPP),
CALOR April Algorithms for the DØ Calorimeter Sophie Trincaz-Duvoid LPNHE – PARIS VI for the DØ collaboration  Calorimeter short description.
1 D.Chakraborty – VLCW'06 – 2006/07/21 PFA reconstruction with directed tree clustering Dhiman Chakraborty for the NICADD/NIU software group Vancouver.
Status of Reconstruction in sidloi3 Ron Cassell 5/20/10.
Status of the hadronic cross section (small angle) Federico Nguyen February 22 nd 2005  the 2002 data sample and available MC sets  trigger efficiency.
2000/9/23 JPS meeting in Niigata1 Measurement of single gamma and  0 with PHENIX EMCal (I) H.Torii Kyoto Univ./RIKEN for the PHENIX Collaboration. Sep/23/2000,
Fast Simulation and the Higgs: Parameterisations of photon reconstruction efficiency in H  events Fast Simulation and the Higgs: Parameterisations of.
1 1 - To test the performance 2 - To optimise the detector 3 – To use the relevant variable Software and jet energy measurement On the importance to understand.
Calice Meeting Argonne Muon identification with the hadron calorimeter Nicola D’Ascenzo.
Calibration of the ZEUS calorimeter for hadrons and jets Alex Tapper Imperial College, London for the ZEUS Collaboration Workshop on Energy Calibration.
AHCAL analyses overview List of ongoing analyses targeted to the upcoming publications Erika Garutti.
7/13/2005The 8th ACFA Daegu, Korea 1 T.Yoshioka (ICEPP), M-C.Chang(Tohoku), K.Fujii (KEK), T.Fujikawa (Tohoku), A.Miyamoto (KEK), S.Yamashita.
Trigger study on photon slice Yuan Li Feb 27 th, 2009 LPNHE ATLAS group meeting.
Dijet Mass and Calibration1 H C A L Z(700) Data and Calibration Dan Green Fermilab June, 2001.
Régis Lefèvre (LPC Clermont-Ferrand - France)ATLAS Physics Workshop - Lund - September 2001 In situ jet energy calibration General considerations The different.
Feb. 3, 2007IFC meeting1 Beam test report Ph. Bruel on behalf of the beam test working group Gamma-ray Large Area Space Telescope.
Study of Calorimeter performance using the LC full simulator The 8th ACFA Workshop Yoshihiro Yamaguchi (Tsukuba U.) M. -C. Chang (RCNS, Tohoku U.) K. Fujii.
DESY1 Particle Flow Calorimetry At ILC Experiment DESY May 29 th -June 4 rd, 2007 Tamaki Yoshioka ICEPP, Univ. of Tokyo Contents.
John Marshall, 1 John Marshall, University of Cambridge LCD-WG2, July
V. Pozdnyakov Direct photon and photon-jet measurement capability of the ATLAS experiment at the LHC Valery Pozdnyakov (JINR, Dubna) on behalf of the HI.
 reconstruction and identification in CMS A.Nikitenko, Imperial College. LHC Days in Split 1.
Status of the measurement of K L lifetime - Data sample (old): ~ 440 pb -1 ( ) - MC sample: ~125 pb -1 ( mk0 stream ) Selection: standard tag (|
David Lange Lawrence Livermore National Laboratory
Reconstruction of converted photons E. Tournefier LAPP meeting Feb. 2,2012 Algorithm for the reconstruction of converted photons Performances studies:
Multi-lepton and general searches at HERA Andrea Parenti (DESY-Hamburg) on behalf of H1 and ZEUS collaborations - DIS Outline: ● Multi-electron.
Jet Energy Scale and Calibration Framework
ILC Software Meeting, Orsay 05/07
Individual Particle Reconstruction
Argonne National Laboratory
Detector Optimization using Particle Flow Algorithm
LC Calorimeter Testbeam Requirements
Presentation transcript:

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 1 New ideas and old doubts about the calorimeter shaking procedure Andrea Venturi INFN Pisa

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 2 Present status ECAL and HCAL cluster energies are changed according to the observed data vs MC discreapancies as a function of polar angle –qqbar events at Z peak polar angle from jet direction –at a lower level w.r.t. EFLOW because of jet corrections PHCO for HCAL PECO, PEST,ETDI,...for ECAL –number of “raw” clusters is not changed it does not work if this is a relevant discreapancy Results (winter 01) –4q: 9 MeV –electrons: 20 MeV –muons: 5 MeV –taus: 5 MeV The procedure has to be validate “a posteriori” –check “higher level” observables before and after shaking: the changes should be of the level of the discrepancies angular bias visible energy... –understand the results electron/muon difference: brems corr ?

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 3 HCAL shaking data  MC data/MC

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 4 ECAL shaking data/MC data  MC

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 5 PHCO Type 5 (neut had) Eflow ETDI (towers) PECO raw PECO corr. Type 5 (neut had) Photons Type 4 (photons) Eflow Gampex Corrections: leakage overlap cracks …. Coradoc MC  data Platine

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 6 EFLOW energy: jet correction data  MC data  MC

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 7 Higher level observables and shaking no shaking  shaking data  MC (shaken) black : MC (not shaken) blue : MC (shaken) by Ann

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 8 ECAL is not easy ECAL is crucial and the present shaking is not that good: PECO raw vs PECO corrected –data vs MC discrepancies are different –EFLOW (#5) uses PECO corrected –EFLOW (#4) uses GAMPEX same correction as PECO corr. ? –the shaking parameters are taken from PECO raw –Why different discrepancies ? it could be a useful tool to study ECAL simulation discrepancies –What should we use for the shaking ? should we use “shaking” ? PECO corr: data/MC PECO raw: data/MC

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 9 ECAL is not easy (II) Two different processes produce signal in ECAL e.m. interactions (photons, electrons) hadronic interactions (hadrons) –data vs MC discrepancies can be very different –Different shaking based on the particle id (identified photons/electrons) is not enough it does not take into account identification efficiency/purity it is not easy to propagate the shaking back to the “raw” banks –cfr brems correction in lnqq –Ideal: use of the MC history banks are they ok for ECAL ? Discrepancy is larger for type 4 and 5 separately than for the sum –shaking should “migrate” the energy from photons to neutral hadrons and viceversa cfr. my test with modified ECAL noise banks study photon id algorithm to understand how to shake to change the algorithm performance –shake each ECAL stack independently ? MC history banks ? Brems correction (enqq) –have specific studies ever been done ? –check the effect of the shaking

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 10 std ENNO bank new ENNO bank

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 11 Photons: ad hoc corrections Identified photon energies are corrected with corrections (CORADOC) which are different between data and MC –how are they evaluated: pi0’s ? di-muons radiative events ? electrons ? to be asked to MNM…(done!)

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 12 Photons (II) Photons corrections are like jet corrections: –they try to correct for the data vs MC discrepancy –this has to be taken into account in the shaking procedure once the shaking has been applied, new MC photon corrections have to be evaluated and used. not because photons are better !! But, are we sure about the present photon energy corrections: –do we need better correction or tracking resolution problems ?

4/04/2001Calorimeter shaking -Andrea Venturi - April '01 ALEPH week 13 Summary To be understood –PECO: raw vs corrected –noise banks and better agreement: why ? Not to be forgotten –photon energy corrections are not taken into account in shaking neither if they are correct: less discrepancy nor if they are not correct: additional discrepancy To be done –shaking-dependent photon corrections –check observables after shaking e/mu present difference To be checked –have photon corrections to be improved ? –simulation of the electron brems (reconstruction) who knows if it was studied in the early days ?