Validation of DC3 fully simulated W→eν samples (NLO, reconstructed in 11.0.42) Laura Gilbert 01/08/06.

Slides:



Advertisements
Similar presentations
QCD Background… and the Resolution Saminder Dhaliwal August 30 th 2005.
Advertisements

Top Physics Validation: Reconstruction, Simulation and Bytestream Paul S Miyagawa The University of Manchester.
1 N. Davidson E/p single hadron energy scale check with minimum bias events Jet Note 8 Meeting 15 th May 2007.
1 previously, when I calculated event selection efficiencies, I defined efficiencies as the following: efficiency in electron channel = (total number of.
Top Turns Ten March 2 nd, Measurement of the Top Quark Mass The Low Bias Template Method using Lepton + jets events Kevin Black, Meenakshi Narain.
1 Strange Sea Asymmetry Analysis: Update Laura Gilbert 18/09/07.
1 N. Davidson E/p minimum bias update with Athena Analysis Meeting 12 th June 2007.
1 Hadronic In-Situ Calibration of the ATLAS Detector N. Davidson The University of Melbourne.
1 N. Davidson E/p minimum bias update with Athena Jet Note 8 Meeting 7 th June 2007.
1 Andrea Bangert, ATLAS SCT Meeting, Monte Carlo Studies Of Top Quark Pair Production Andrea Bangert, Max Planck Institute of Physics, CSC T6.
1 N. Davidson, E. Barberio E/p single hadron energy scale check with minimum bias event Hadronic Calibration Workshop 26 th -27 th April 2007.
A Feasibility Study on Measuring a Strange Sea Asymmetry in the Proton 14/07/05Laura Gilbert, Jeff Tseng.
A simulation study of the rapidity distributions of leptons from W boson decays at ATLAS Laura Gilbert.
1 A Feasibility Study for a Strange Sea Asymmetry Analysis at ATLAS: update II Laura Gilbert and Jeff Tseng 13/12/07.
Analysis Meeting – April 17 '07 Status and plan update for single hadron scale check with minimum bias events N. Davidson.
Single Top Trigger Studies Top Trigger Meeting, 9 May Patrick Ryan, MSU Single Top Trigger Studies Top Trigger Meeting 9 May 2007 Patrick Ryan.
1 N. Davidson Calibration with low energy single pions Tau Working Group Meeting 23 rd July 2007.
Study of DC3 Fully Simulated W→eν Samples with an eye to Strange Sea Asymmetry Analysis Laura Gilbert, University of Oxford 20/09/06 Many thanks to: Jeff.
Energy Flow and Jet Calibration Mark Hodgkinson Artemis Meeting 27 September 2007 Contains work by R.Duxfield,P.Hodgson, M.Hodgkinson,D.Tovey.
W  eν The W->eν analysis is a phi uniformity calibration, and only yields relative calibration constants. This means that all of the α’s in a given eta.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
10 TeV Updates on Efficiencies and Event Shapes Ken Johns, Venkat Kaushik, Xiaowen Lei (U. Arizona) Single lepton + jets channel.
Associated top Higgs search: with ttH (H  bb) Chris Collins-Tooth, 17 June 2008.
2004 Xmas MeetingSarah Allwood WW Scattering at ATLAS.
Lepton efficiency & fake rate Yousuke Kataoka University of Tokyo Content definitions of leptons p2 efficiency and fake rate for SU3 ( ) p3, p4.
19/07/20061 Nectarios Ch. Benekos 1, Rosy Nicolaidou 2, Stathes Paganis 3, Kirill Prokofiev 3 for the collaboration among: 1 Max-Planck-Institut für Physik,
AcerMC and ISR/FSR systematics at ATLAS Liza Mijovic, Borut Kersevan Jozef Stefan Inst. Univ. of Ljubljana ATLAS approach: Generator level studies Parameters.
A few slides to summarise what Alessandro and I were up to for March 24th video meeting Taking for granted that W+/- are good measurements to make- are.
Marco Delmastro 23/02/2006 Status of LAr EM performance andmeasurements fro CTB1 Status of LAr EM performance and measurements for CTB Overview Data -
August 30, 2006 CAT physics meeting Calibration of b-tagging at Tevatron 1. A Secondary Vertex Tagger 2. Primary and secondary vertex reconstruction 3.
Commissioning Studies Top Physics Group M. Cobal – University of Udine ATLAS Week, Prague, Sep 2003.
CaloTopoCluster Based Energy Flow and the Local Hadron Calibration Mark Hodgkinson June 2009 Hadronic Calibration Workshop.
Study of Standard Model Backgrounds for SUSY search with ATLAS detector Takayuki Sasaki, University of Tokyo.
FIMCMS, 26 May, 2008 S. Lehti HIP Charged Higgs Project Preparative Analysis for Background Measurements with Data R.Kinnunen, M. Kortelainen, S. Lehti,
Status of RPC trigger analysis and Muon Trigger efficiencies for W-> μν study By Archana Sharma, Suman B. Beri Panjab University Chandigarh India-CMS Meeting.
Trigger validation for Many thanks to Long Zhao, Chihiro Omachi, Julie Kirk, Giovanni Siragusa, Patricia Conde Muiño, Andreas Reinsch, Olya Igonkina,
Update on Diffractive Dijet Production Search Hardeep Bansil University of Birmingham Birmingham ATLAS Weekly Meeting 13/09/2012.
PFAs – A Critical Look Where Does (my) SiD PFA go Wrong? S. R. Magill ANL ALCPG 10/04/07.
CALOR April Algorithms for the DØ Calorimeter Sophie Trincaz-Duvoid LPNHE – PARIS VI for the DØ collaboration  Calorimeter short description.
Software offline tutorial, CERN, Dec 7 th Electrons and photons in ATHENA Frédéric DERUE – LPNHE Paris ATLAS offline software tutorial Detectors.
Study of pair-produced doubly charged Higgs bosons with a four muon final state at the CMS detector (CMS NOTE 2006/081, Authors : T.Rommerskirchen and.
Status of the hadronic cross section (small angle) Federico Nguyen February 22 nd 2005  the 2002 data sample and available MC sets  trigger efficiency.
1 Update on tt-bar signal and background simulation Stan Bentvelsen.
Fast Simulation and the Higgs: Parameterisations of photon reconstruction efficiency in H  events Fast Simulation and the Higgs: Parameterisations of.
B. Resende Top WG 28/10/05 Polarization studies in ttbar events 1 Polarization studies in tt events with full simulation 1.Physics motivations 2.Full simulation.
Issues with cluster calibration + selection cuts for TrigEgamma note Hardeep Bansil University of Birmingham Birmingham ATLAS Weekly Meeting 12/08/2010.
28/4/2006Chris Collins-Tooth tth, (h → bb) with EventViews Chris Collins-Tooth, Christian Shaw 03-May-2006.
A search for the ZZ signal in the 3 lepton channel Azeddine Kasmi Robert Kehoe Southern Methodist University Thanks to: H. Ma, M. Aharrouche.
Update on Diffractive Dijets Hardeep Bansil University of Birmingham 12/07/2013.
L1Calo EM Efficiencies Hardeep Bansil University of Birmingham L1Calo Joint Meeting, Stockholm 29/06/2011.
Trigger study on photon slice Yuan Li Feb 27 th, 2009 LPNHE ATLAS group meeting.
Régis Lefèvre (LPC Clermont-Ferrand - France)ATLAS Physics Workshop - Lund - September 2001 In situ jet energy calibration General considerations The different.
10 January 2008Neil Collins - University of Birmingham 1 Tau Trigger Performance Neil Collins ATLAS UK Physics Meeting Thursday 10 th January 2008.
Update on Diffractive Dijet Production Search Hardeep Bansil University of Birmingham 23/07/2012.
Update on Diffractive Dijets Search Hardeep Bansil University of Birmingham SM Soft QCD meeting 12/12/2011.
Using direct photons for L1Calo monitoring + looking at data09 Hardeep Bansil University of Birmingham Birmingham ATLAS Weekly Meeting February 18, 2010.
Electron Identification Efficiency from Z→ee Maria Fiascaris University of Oxford In collaboration with Tony Weidberg and Lucia di Ciaccio ATLAS UK SM.
Atautau  lh Carlos Solans TileCal Valencia meeting 20th September 2007.
Electron and Photon HLT alley M. Witek K. Senderowska, A. Żurański.
LNF 12/12/06 1 F.Ambrosino-T. Capussela-F.Perfetto Update on        Dalitz plot slope Where we started from A big surprise Systematic checks.
H->WW->lνlν Analysis - Improvements and results - - Data and MC - Higgs Working group meeting, 6 January 2011 Magda Chełstowska & Rosemarie Aben.
Laura Gilbert, University of Oxford 20/09/06
Missing ET with the First Data: Wl (l=e,)
Venkat Kaushik, Jae Yu University of Texas at Arlington
Higgs → t+t- in Vector Boson Fusion
PDF Uncertainties on W+Jets
semileptonic ttbar + jet events
EM Linearity using calibration constants from Geant4
Plans for checking hadronic energy
tth, (h→bb) with EventViews
Presentation transcript:

Validation of DC3 fully simulated W→eν samples (NLO, reconstructed in ) Laura Gilbert 01/08/06

W→eν from full sim Original sample submitted for generation in December, some of the one million W→e - ν now fully simulated on the grid, in batches of 10k events. Original sample submitted for generation in December, some of the one million W→e - ν now fully simulated on the grid, in batches of 10k events events available (using CBNTs) events available (using CBNTs) Lepton generator level filter efficiency (10Gev, |η|<2.7) was ~63.3% Lepton generator level filter efficiency (10Gev, |η|<2.7) was ~63.3% Generated cross section is 8.4nb (cf. 30nb for W→l - ν: TDR). Luminosity for 10k events is 1.9pb -1. Generated cross section is 8.4nb (cf. 30nb for W→l - ν: TDR). Luminosity for 10k events is 1.9pb -1. Cuts applied at any stage are listed on top right of slide. Cuts applied at any stage are listed on top right of slide. ALL truth plots are normalised to weighting of simulated data EXCEPT multiplicity plots. ALL truth plots are normalised to weighting of simulated data EXCEPT multiplicity plots.

ELECTRONS - truth - full sim Sanity plots: multiplicity

Electron Selection Cuts At least one electron with transverse energy > 25GeV. (Use ET rather than pT since brem recovery not properly implemented yet0 At least one electron with transverse energy > 25GeV. (Use ET rather than pT since brem recovery not properly implemented yet0 Electron candidate has at least one associated track matched (exclude photons) Electron candidate has at least one associated track matched (exclude photons) η < 2.4. This cuts out dubious candidates at the end of the electromagnetic calorimeter. η < 2.4. This cuts out dubious candidates at the end of the electromagnetic calorimeter. IsEM flag = 0, electron isolation cut. This should now be tuned correctly but I need to look into the bitwise cuts in more detail to check. IsEM flag = 0, electron isolation cut. This should now be tuned correctly but I need to look into the bitwise cuts in more detail to check.

ELECTRONS - truth - full sim Sanity plots: multiplicity of electrons that pass selection cuts Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4 Almost always only one electron candidate per event passes cuts.

ELECTRONS Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4 Checking cuts with truth info: - before cuts - after cuts Initially tracks of candiadates entered into egamma container include kaons, pions, muons. After cuts only electrons remain.

ELECTRONS Sanity plots: phi - truth - full sim Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4

ELECTRONS Sanity plots: eta - truth - full sim Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4

ELECTRONS Identifying electrons with their partner in truth containers, matching (η,φ) space: If (ΔR<0.1) match is found Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4

ELECTRONS Sanity plots: ET - truth - full sim Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4

ELECTRONS Difference between simulated and truth ET distributions: No overall difference between simulated and truth ET shapes! PROBLEM? Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4

ELECTRONS Electron ET resolution: (sim-truth)/truth for matched sim:truth electron pairs. Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4 ΔR<0.1 (matching sim to truth) Resolution looks roughly ok though…

ELECTRONS "Wrong sign" electrons found from associated track q/p, AFTER cuts: Wrong signCorrect sign *PROBLEM* Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4

ELECTRONS ET distribution of "wrong sign" electron candidates: - +ve charge electrons (from track q/p) - all electron candidates (for shape comparison) Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4

ELECTRONS Consider truth information: just cut on ET > 25GeV - before cuts - after cuts There are positrons present in egamma truth, but none pass ET cut. Cuts: ET (ele truth) > 25GeV

ELECTRONS What are the wrong sign electrons? What are the wrong sign electrons? Not generated positrons Not generated positrons Don't have high pT tracks, so probably not electrons mis-reconstructed. Don't have high pT tracks, so probably not electrons mis-reconstructed. Possibly wrong track-cluster combinations. Needs further investigation. Possibly wrong track-cluster combinations. Needs further investigation.

Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 η(ele) < 2.4 ELECTRON ISSUES E over p always 0! → needs to be fixed in future. Where do the "positrons" come from? Need to look into IsEM flags in detail. Further investigation needed:

ELECTRON JETS W Transverse mass plots look fishy if I apply exclusions on events containing jets with ET>30GeV. Therefore many jets come from electrons. Identify and exclude these electron jets. Can only be one on jets with η<2.5 to make electron matching possible. (Jets reconstructed using cone algorithm with R<0.7, see later)

ELECTRON JETS Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 Jet η < 2.5 Identify jets with electrons if ΔR<0.7 - truth - full sim Matching electrons and jets in (η,φ) space: Log scale→

ELECTRON JETS Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 Jet η < 2.4 Jets are corrected to have more energy than electron candidates so -ve values more likely to be a match. Trying to match energy as well as (η,φ) distribution (no cut made): - truth - full sim Matching electrons and jets in energy:

ELECTRON JETS Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 Jet η < 2.4 A closer look at electron-jet ΔR and energy distributions: simulation Smattering of events here

ELECTRON JETS Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 Jet η < 2.4 A closer look at electron-jet ΔR and energy distributions: truth no events here

ELECTRON JETS Cuts: ET(ele) > 25GeV At least one track matched IsEM=0 Jet η < 2.4 A closer look at electron-jet ΔR and energy distributions: (truth - simulation) This is the normalised difference of the last two plots! ΔRΔR Energy difference (MeV) Truth - simulated

JETS Cuts: ΔR (e-jet) > 0.7 Jet η < 2.4 Looking at all jets which have not been matched with electrons: ie. Jets which are isolated from electron candidates by at least 0.7 in (η,φ). Looking at all jets which have not been matched with electrons: ie. Jets which are isolated from electron candidates by at least 0.7 in (η,φ). Still looking at jets with η<2.4 for accurate electron matching. Still looking at jets with η<2.4 for accurate electron matching. There are three available clustering algorithms: There are three available clustering algorithms: Kt alorithm: apparently unsuitable for low pT jets. Kt alorithm: apparently unsuitable for low pT jets. Cone algorithm with R<0.4. Discounted as produces very low statistics (few jets reconstructed) Cone algorithm with R<0.4. Discounted as produces very low statistics (few jets reconstructed) Cone algorithm with R<0.7. Use this. Cone algorithm with R<0.7. Use this.

JETS Sanity plots: multiplicity before any selection: - truth - full sim

JETS Cuts: ΔR (e-jet) > 0.7 Jet η < 2.4 Sanity plots: multiplicity after electron/jet matches removed, jet η<2.4 - truth - full sim Log scale→ Multiplicity greatly reduced

JETS Sanity plots: phi Cuts: ΔR (e-jet) > 0.7 Jet η < truth - full sim

JETS Sanity plots: eta Shape before η cut Cuts: ΔR (e-jet) > 0.7 Jet η < truth - full sim

JETS Cuts: ΔR (e-jet) > 0.7 Jet η < 2.4 ΔR(jet-truth)<0.5 Matching jets with truth in (η,φ) space: Log scale→ If (ΔR<0.5) match is found

JETS Sanity plots: ET Cuts: ΔR (e-jet) > 0.7 Jet η < truth - full sim Jets not reconstructed < 10GeV

JETS ET resolution: (sim-truth)/truth Cuts: ΔR (e-jet) > 0.7 Jet η < 2.4 ΔR(jet-truth)<0.5

JETS Sanity plots: Energy Cuts: ΔR (e-jet) > 0.7 Jet η < truth - full sim

JETS Energy resolution: (sim-truth)/truth Cuts: ΔR (e-jet) > 0.7 Jet η < 2.4 ΔR(jet-truth)<0.5

JETS Sanity plots: ET Cuts: ΔR (e-jet) > 0.7 Jet η < truth - full sim Strange: data is shifted down from truth.

JET ISSUES Jets from electrons are easily identified and removed by an exclusion cut in (η,φ) space. Jets from electrons are easily identified and removed by an exclusion cut in (η,φ) space. Not certain this is the best algorithm, but other available algorithms have more problems. Not certain this is the best algorithm, but other available algorithms have more problems. Jet statistics low after removal of electrons, therefore resolutions not well defined. Jet statistics low after removal of electrons, therefore resolutions not well defined. Meaning of jet “mass” not well understood, left- shift of simulation w.r.t. truth unexpected. Meaning of jet “mass” not well understood, left- shift of simulation w.r.t. truth unexpected.

MISSING ENERGY - truth: calculated from non- interacting particles - full sim: corrected, inc. muons Sanity plots: Missing ET Probably not properly calibrated Cuts: Ptele > 25GeV At least one track matched IsEM=0 Electron η < 2.4 Jet η < 2.4 ΔR (e-jet) > 0.7 MET>25GeV Cut on MET>25GeV

MISSING ENERGY Cuts: Ptele > 25GeV At least one track matched IsEM=0 Electron η < 2.4 Jet η < 2.4 ΔR (e-jet) > 0.7 MET>25GeV Missing ET Resolution: Asymmetry reflecting right-shift of data w.r.t. truth

MISSING ENERGY - truth - full sim Cuts: Ptele > 25GeV At least one track matched IsEM=0 Electron η < 2.4 Jet η < 2.4 ΔR (e-jet) > 0.7 MET>25GeV Missing ET φ distribution:

W RECONSTRUCTION - truth - full sim Cuts: Ptele > 25GeV At least one track matched IsEM=0 Electron η < 2.4 Jet η < 2.4 ΔR (e-jet) > 0.7 MET>25GeV W transverse mass reconstructed from Missing ET and highest ET electron:

Conclusions: The W looks like TDR (right)! The W looks like TDR (right)! Electrons are well reconstructed. Electrons are well reconstructed. The e/p variable in the egamma container should probably be fixed. The e/p variable in the egamma container should probably be fixed. Electrons with mis-identified charge not yet understood. Electrons with mis-identified charge not yet understood. Missing energy doesn’t seem best corrected to match truth. Missing energy doesn’t seem best corrected to match truth. Insufficient stats for decent jet resolution. Insufficient stats for decent jet resolution. Jet “mass” shift seems strange. Jet “mass” shift seems strange.