1 Top activities in Milano. 2 Overview Study of W+jets background to semileptonic tt –I. Besana (1 st year PhD student, continuing work of diploma thesis)

Slides:



Advertisements
Similar presentations
Current limits (95% C.L.): LEP direct searches m H > GeV Global fit to precision EW data (excludes direct search results) m H < 157 GeV Latest Tevatron.
Advertisements

Tau dilepton channel The data sample used in this analysis comprises high-p T inclusive lepton events that contain an electron with E T >20 GeV or a muon.
The Matrix Method Data-driven method of estimating the W→lv and QCD multijet contributions to sample S’.
Introduction to Single-Top Single-Top Cross Section Measurements at ATLAS Patrick Ryan (Michigan State University) The measurement.
1 Measuring the Top Quark Cross Section in the Semileptonic Channel Andrea Bangert.
1 A limit on Br(t→Zc) Henry Frisch, Carla Pilcher, Collin Wolfe, Alexander Paramonov VEP Meeting June 19, 2007.
Heavy charged gauge boson, W’, search at Hadron Colliders YuChul Yang (Kyungpook National University) (PPP9, NCU, Taiwan, June 04, 2011) June04, 2011,
H → ZZ →  A promising new channel for high Higgs mass Sara Bolognesi – Torino INFN and University Higgs meeting 23 Sept – CMS Week.
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.
Analysis Plans for Jets + EtMiss Signatures Pierre Savard ATLAS Toronto Group Meeting January
W+jets and Z+jets studies at CMS Christopher S. Rogan, California Institute of Technology - HCP Evian-les-Bains Analysis Strategy Analysis Overview:
Study of the to Dilepton Channel with the Total Transverse Energy Kinematic Variable Athens, April 17 th 2003 Victoria Giakoumopoulou University of Athens,
Sensitivity Prospects for Light Charged Higgs at 7 TeV J.L. Lane, P.S. Miyagawa, U.K. Yang (Manchester) M. Klemetti, C.T. Potter (McGill) P. Mal (Arizona)
LHC France 2013, 3 rd April ATLAS results on inclusive top quark pair production cross section in dilepton channel Frédéric Derue, LPNHE Paris Rencontres.
Possibility of tan  measurement with in CMS Majid Hashemi CERN, CMS IPM,Tehran,Iran QCD and Hadronic Interactions, March 2005, La Thuile, Italy.
1 ttbar Cross-Section Studies D. Jana*, M. Saleem*, F. Rizatdinova**, P. Gutierrez*, P. Skubic* *University of Oklahoma, **Oklahoma State University.
Liu Minghui Nanjing MC study of W polarization and ttbar spin correlation Liu Minghui, Zhu Chengguang April 27, 2008.
1 Single top in e+jets channel Outline : - Data and MC samples - Overview of the analysis - Loose and topological cuts - MC efficiencies and expected number.
Slides for EB3. Left Problems from EB2 1. Why muon triggers are not used in e  channel? 2. Add backgrounds estimation for signal search region 3. Add.
28/01/101 Zvv bkg, how to get an estimate with first data ? R. Brunelière Time schedule is tight. Goal : get an estimate by may/june if we get data from.
ATLAS Higgs Search Strategy and Sources of Systematic Uncertainty Jae Yu For the ATLAS Collaboration 23 June, 2010.
Kinematics of Top Decays in the Dilepton and the Lepton + Jets channels: Probing the Top Mass University of Athens - Physics Department Section of Nuclear.
La Thuile, March, 15 th, 2003 f Makoto Tomoto ( FNAL ) Prospects for Higgs Searches at DØ Makoto Tomoto Fermi National Accelerator Laboratory (For the.
Z  BF using  hadronic events Silke Duensing Aug 8th, 2003.
1 UCSD Meeting Calibration of High Pt Hadronic W Haifeng Pi 10/16/2007 Outline Introduction High Pt Hadronic W in TTbar and Higgs events Reconstruction.
News from H->bb Ricardo Gonçalo on behalf of H->bb Note group HSG5 Meeting – 3 Dec
Top physics at startup CMS France – 1 er avril 2010 Anne-Catherine Le Bihan.
Lorenzo Bellagamba, Graziano Bruni, Riccardo Di Sipio (Bologna); Ilaria Besana, Tommaso Lari, Clara Troncon (Milano); Bobby Acharya, Marina Cobal, Umberto.
W→e and W→e +jets: a data-driven selection method By Alessandro Tricoli ATLAS UK SM Meeting 4 th June 2008 In Collaboration with M. Wielers (RAL) D. Prieur.
Measuring the t-tbar Cross-Section in the Dilepton Channel at CDF* J. Incandela for C. Mills Jan. 17, 2008 DOE Site Visit UC Santa Barbara * PhD Thesis.
Search for Pair Produced Stops Decaying to a Dileptonic Final State at CMS David Kolchmeyer.
Search for Standard Model Higgs in ZH  l + l  bb channel at DØ Shaohua Fu Fermilab For the DØ Collaboration DPF 2006, Oct. 29 – Nov. 3 Honolulu, Hawaii.
A Search for Higgs Decaying to WW (*) at DØ presented by Amber Jenkins Imperial College London on behalf of the D  Collaboration Meeting of the Division.
Status of the Higgs to tau tau analysis Carlos Solans Cristobal Cuenca.
Top Full simulation study B. Zilka, S.Tokar Comenius University, Bratislava.
Data Driven study for Same Sign Dileptons July 31 st 2009, “CMS SUSY Leptonic Meeting” 1 Sanjay Padhi.
Top quark pair cross-section D0 (1 fb -1 results) Viatcheslav Sharyy for D0 collaborations CEA-Saclay / IRFU/ SPP ● Introduction ● Dilepton.
Slide 1 Status Report. Slide 2 QCD and W+jets Background Estimation Using Fake Rate Method Norbert Neumeister, Hwidong Yoo Purdue University EXO non-hadronic.
ATLAS results on inclusive top quark pair
Status of the Higgs to tau tau
The Top Quark at CDF Production & Decay Properties
Update on Invisible Higgs analysis in the tth channel
15/11/11 LHCb Liverpool Meeting
Report from SUSY working group
Tracking performances & b-tagging commissioning
Missing ET with the First Data: Wl (l=e,)
Measurement of SM V+gamma by ATLAS
on top mass measurement based on B had decay length
Early EWK/top measurements at the LHC
SUSY Particle Mass Measurement with the Contransverse Mass Dan Tovey, University of Sheffield 1.
CDS comments on supporting note
Top quark search update
Stop->4 bodies signal samples with 2 leptons in final state
Higgs → t+t- in Vector Boson Fusion
D3PDs production+validation, preliminary TeV
NIKHEF / Universiteit van Amsterdam
W boson helicity measurement
Top Quark Production at the Large Hadron Collider
Prospects for sparticle reconstruction at new SUSY benchmark points
Jessica Leonard Oct. 23, 2006 Physics 835
-signals and background for new physics searches-
Searches at LHC for Physics Beyond the Standard Model
W/Z+jets Background Determination in the ATLAS ICHEP SUSY Notes
W/Z and Di-Boson Results from ATLAS Srivas Prasad Harvard University On behalf of the ATLAS Collaboration Pheno Madison, Wisconsin May 09, 2011.
ttbar + jets AOD analysis
W/Z and Di-Boson Results from ATLAS Srivas Prasad Harvard University On behalf of the ATLAS Collaboration Pheno Madison, Wisconsin May 09, 2011.
The others’ latest result about SUSY search with same-sign dimuon
C.M.S.:.
Northern Illinois University / NICADD
Presentation transcript:

1 Top activities in Milano

2 Overview Study of W+jets background to semileptonic tt –I. Besana (1 st year PhD student, continuing work of diploma thesis) Study of Z(  ) background to double leptonic tt –M.C.Conidi (diploma student) and L. Dell’Asta (2 nd year PhD student) Study of b-tagging in ttbar events –S. Montesano (3 rd year PhD student) –See next talk One of the main goals of Milano is the search for supersymmetry Requires energy/luminosity, and well understood detector/backgrounds For 2009, main effort will be on ttbar and relative backgrounds

3 W+jets analysis goals In order of increasing luminosity we would like to Select event with one lepton and MET, see W over QCD. Need a QCD estimate - for example, from jet stream with non isolated leptons, normalizing at low MT or MET Measure W/Z ratio for low jet multeplicity (0, 1, 2? jets) and compare with MC predictions From measured Z+jets (high jet multeplicity as in ttbar selection), measured W/Z ratio at low jet multiplicity, and (small) MC corrections, predict W+jets background. c is a coefficient taking into account mass difference between W and Z Compare with estimate using W+jets MC normalized at low jet multiplicity. Contribute to first ttbar cross section measurement in semileptonic channel The first point is doable even with very low luminosity/energy Need to decide wether to focus on electron or muon channel

4 W+jets release 12 studies some ambiguity in the normalization of alpgen data (samples had a jet filter) All numbers for 100 pb -1 Ilaria’s presentations at SM and top meetings: Other studies: LBNL, ATLAS-COM , Generator-level studies with several MC Marisa Sandhorf (Wuppertal) I. Besana, diploma thesis

5 Ongoing work Use mc08 data –Migrate analysis code from custom ntuples produced from rel12 AOD to Athena-based analysis in release 14. Repeat W/Z ratio studies done with CSC data, then go beyond -Systematics (at generator-level, comparing different programs and tunings, and at detector-level) -Offline and trigger selection -Select W and remove/estimate QCD with very early data -Can we measure W+1jet/Z+1jet and constrain generator predictions? Top contamination with 2 jets? -How does it compare with just using W+jets MC predictions normalized to low jet multiplicity bins ?

6 Z(  ) and top Events rates after di-leptonic top selection (Maria Chiara thesis, 1000 pb -1 at 14 TeV) Z(  ) with di-leptonic tau decay is an important background to dilepton top searches Idea: estimate it from a Z(  ) control sample, replacing the two muons with a Z->  ->  simulated decay - jets, underlying event and Z momentum is taken from the data - Z decay simulation is MC (reliable) Similar to the technique used to estimate the Z background to H->  ->ll signal (see CSC book). 2 jets pt > 35 GeV EtMiss > 30 GeV (50 GeV for e  ) 2 isolated leptons pt>15 GeV Invariant mass outside [80 GeV,100 GeV] CSC trigger menu M.C. Conidi, diploma thesis

7 Z(  ) estimate - technique a) Select Z(  ) from data (98% purity) b) Simulate a Z decay in its rest frame - generate the two muons energy and relative angle according to 3-dimensional reference distributions from Z(  ) MC sample - 3 other angles assumed isotropic (need to check effect of Z polarization, if any) c) Use the measured Z velocity to go back to ATLAS frame d) Replace the two original muons with the simulated decay, recompute EtMiss, simulate muon trigger+reco efficiency 2 opposite charge muons 80 GeV < m inv < 100 GeV 2 or more jets with p T >20GeV No requirment on E T miss Single Muon Trigger (mu20)

8 Massa invariante dei μ in eventi Z  ττ MC (in blu) e in eventi Z  ττ  μμ+4ν simulati (in verde), dopo aver applicato i criteri di selezione su p T dei getti, missing E T ed energia di isolamento. Energia del μ + in eventi Z  ττ MC (in blu) e in eventi Z  ττ  μμ + 4ν simulati (in verde). Cut on MC truth info saved in TopView ntuples Technique seems to work. Need much more MC events to assess precision (Alpgen statistics with loose filter very limited in release 12) Some aproximations (constant muon efficiency, isotropic muon decay) need to be improved. Z(  ) estimate - results

9 Z(  ) future developments Maria Chiara gets her degree next week. Lidia may continue her work –Move code from ROOT macros to ATHENA. Replacement of part of a real event with a simulated Z decay should become a public tool –Repeat analysis with mc08 and mc09 data (MC statistics much better by the way). Improve analysis as mentioned; evaluate systematics We are however discussing if the Z(  ) background is the best usage of this tool with early data –With ~2 pb -1 at 10 TeV, 10 signal events and ~0.2 Z(  ) background events – do we need a data-driven background estimate? –An other possible application of the tool would be replace an hadronic tau instead, generate W(  ) from W(l ) control sample, compare with W(  ) signal and measure tau trigger and reconstruction efficiency