B Tagging Efficiency and Mistag Rate Measurement in ATLAS

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

Search for Top Flavor Changing Neutral Current Decay t → qZ Ingyin Zaw DOE Review August 21, 2006.
Gavril Giurgiu, Carnegie Mellon 1 B s Mixing at CDF Seminar at Fermi National Accelerator Laboratory Gavril Giurgiu Carnegie Mellon University August 16,
1 B-tagging meeting overview Li bo Shandong University.
BRING UP B-TAGGING AT DØ Gordon Watts (Seattle/Marseille)
ICFP 2005, Taiwan Colin Gay, Yale University B Mixing and Lifetimes from CDF Colin Gay, Yale University for the CDF II Collaboration.
The Matrix Method Data-driven method of estimating the W→lv and QCD multijet contributions to sample S’.
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.
Kevin Black Meenakshi Narain Boston University
MC Study on B°  S (Status Report) Jianchun Wang Syracuse University BTeV meeting 05/25/01.
Introduction to Single-Top Single-Top Cross Section Measurements at ATLAS Patrick Ryan (Michigan State University) The measurement.
Top Mass Measurement at the Tevatron HEP2005 Europhysics Conference Lisboa, Portugal, June 22, 2005 Koji Sato (Univ. of Tsukuba) for CDF and D0 Collaborations.
1 Viktor Veszprémi (Purdue University, CDF Collaboration) SUSY 2005, Durham Search for the SM Higgs Boson at the CDF Experiment Search for the SM Higgs.
Single-Top Cross Section Measurements at ATLAS Patrick Ryan (Michigan State University) Introduction to Single-Top The measurement.
Chris Barnes, Imperial CollegeWIN 2005 B mixing at DØ B mixing at DØ WIN 2005 Delphi, Greece Chris Barnes, Imperial College.
Radiative Leptonic B Decays Edward Chen, Gregory Dubois-Felsmann, David Hitlin Caltech BaBar DOE Presentation Aug 10, 2005.
Measurement of the Branching fraction B( B  D* l ) C. Borean, G. Della Ricca G. De Nardo, D. Monorchio M. Rotondo Riunione Gruppo I – Napoli 19 Dicembre.
Associated top Higgs search: with ttH (H  bb) Chris Collins-Tooth, 17 June 2008.
Z AND W PHYSICS AT CEPC Haijun Yang, Hengne Li, Qiang Li, Jun Guo, Manqi Ruan, Yusheng Wu, Zhijun Liang 1.
B-tagging Performance based on Boosted Decision Trees Hai-Jun Yang University of Michigan (with X. Li and B. Zhou) ATLAS B-tagging Meeting February 9,
Section of experimental particle physics Per Hansson Top D0 Summer Physics Workshop June Top Charge Measurement using Jet Charge Templates.
Gavril Giurgiu, Carnegie Mellon, FCP Nashville B s Mixing at CDF Frontiers in Contemporary Physics Nashville, May Gavril Giurgiu – for CDF.
August 30, 2006 CAT physics meeting Calibration of b-tagging at Tevatron 1. A Secondary Vertex Tagger 2. Primary and secondary vertex reconstruction 3.
HERA-LHC, CERN Oct Preliminary study of Z+b in ATLAS /1 A preliminary study of Z+b production in ATLAS The D0 measurement of  (Z+b)/  (Z+jet)
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.
Measurement of b-tagging Fake rates in Atlas Data M. Saleem * In collaboration with Alexandre Khanov** F. Raztidinova**, P.Skubic * *University of Oklahoma,
Searches for the Standard Model Higgs at the Tevatron presented by Per Jonsson Imperial College London On behalf of the CDF and DØ Collaborations Moriond.
B-Tagging Algorithms for CMS Physics
1 TOP2006 Workshop Coimbra, Portugal Jan,2006 Top quark reconstruction in ATLAS V. Kostyukhin INFN Genova on behalf of ATLAS collaboration.
Update on H→WW→2μ2ν Update on H→WW→2μ2ν Oct. 8, 2010 IFCA – U. Oviedo.
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.
Jet Prob optimization for the s-channel search Hideki Maehashi University of Tsukuba 7/28/2008 Contents 1.Single Top Search 2.Jet Probability 3.Event Selection.
Julien Donini University of Padova and INFN  Jet energy scale issues  Understanding our dataset  Z  bb signal extraction  What's next Tev4LHC at CERN.
Susan Burke DØ/University of Arizona DPF 2006 Measurement of the top pair production cross section at DØ using dilepton and lepton + track events Susan.
Single top quark physics Peter Dong, UCLA on behalf of the CDF and D0 collaborations Les Rencontres de Physique de la Vallee d’Aoste Wednesday, February.
Moriond QCD March 24, 2003Eric Kajfasz, CPPM/D01 b-production cross-section at the TeVatron Eric Kajfasz, CPPM/D0 for the CDF and D0 collaborations.
B-Tagging Algorithms at the CMS Experiment Gavril Giurgiu (for the CMS Collaboration) Johns Hopkins University DPF-APS Meeting, August 10, 2011 Brown University,
Jessica Levêque Rencontres de Moriond QCD 2006 Page 1 Measurement of Top Quark Properties at the TeVatron Jessica Levêque University of Arizona on behalf.
Viktor Veszpremi Purdue University, CDF Collaboration Tev4LHC Workshop, Oct , Fermilab ZH->vvbb results from CDF.
DPF Conf., Oct. 29, 2006, HawaiiViktor Veszpremi, Purdue U.1 Search for the SM Higgs Boson in the Missing E T + b-jets Final State at CDF V. Veszpremi.
VHF working meeting, 4 Oct Measurement of associated charm production in W final states at  s=7TeV J. Alcaraz, I. Josa, J. Santaolalla (CIEMAT,
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.
QCD estimate with the matrix method Alexander D. with the help of many…
Les Houches Workshop, Marco Zanetti - INFN Padova H->WW->2l: general properties High  *BR higgs channel, but no peak! To understand the backgrounds the.
Top Full simulation study B. Zilka, S.Tokar Comenius University, Bratislava.
Exploring Artificial Neural Networks to Discover Higgs at LHC Using Neural Networks for B-tagging By Rohan Adur
ATLAS results on inclusive top quark pair
Erik Devetak Oxford University 18/09/2008
Using IP Chi-Square Probability
on top mass measurement based on B had decay length
SUSY Particle Mass Measurement with the Contransverse Mass Dan Tovey, University of Sheffield 1.
Venkat Kaushik, Jae Yu University of Texas at Arlington
2vtx tagged dijets mass resolution study
An Important thing to know.
W Charge Asymmetry at CDF
W boson helicity measurement
Top Quark Production at the Large Hadron Collider
b-tagging commissioning strategy for ATLAS
b-tagging commissioning strategy at ATLAS
Searches at LHC for Physics Beyond the Standard Model
Prospects for quarkonium studies at LHCb
Heavy Flavour Content of the Proton
Tim Scanlon Imperial College, London on behalf of the DØ Collaboration
b-tagging efficiency in L+jets at 7TeV
A brief update on b-tagging of High P jets
Susan Burke, University of Arizona
Northern Illinois University / NICADD
Study of Top properties at LHC
Measurement of b-jet Shapes at CDF
Presentation transcript:

B Tagging Efficiency and Mistag Rate Measurement in ATLAS Thomas Delemontex (LPSC) Jin Wang (Shandong University && LPSC)

Objective and Motivation B Jet Identification Light Jet Mistag Rate B Tagging Efficiency B Tagging Efficiency B Tagging Efficiency Light Jet Mistag Rate W+jets events QCD events W+jets events QCD events

B-tagging Algorithm B-tagging algorithms are used to tag the b-jets originating from b quarks. In first data, three algorithms are going to be used: TrackCounting: use tracks with large impact parameter. JetProb: calculate the probability of a track to be from light jet. Secondary Vertex Reconstruction (SV0): use the signed decay length significance of the secondary vertex .

Definition Each tagger provides a tag weight w. On this w distribution of all reconstructed jets, we cut at certain threshold , and define : B-tagging efficiency : Mistag rate : Light jet rejection : rejection =

B tag efficiency measurement : pTRel method (1/2) Definition : for a muonic jet, it’s the transverse momentum of the muon compared to the jet axis CSC Note: CERN-OPEN-2008-020 Jet axis Soft muon PT Form CSC note θμ-jet Primary vertex pTRel is sensitive to jet flavors

B tag efficiency measurement : pTRel method (2/2) Simply a fit of an unknown pTRel distribution with previous templates Form CSC note Jet sample without any btag requirement Adjustment of template normalizations We find nb jets in this sample Same sample with a btag requirement We find ntaggedb jets in this sample Form CSC note B tagging efficiency is a simple ratio

pTRel method : Results Form CSC note - pTrel method is OK up to 80 GeV and then becomes less efficient due to similarities between light, c and b templates - Soon dominated by systematic uncertainties (fragmentation function used, muon pT measurement , misalignment …) - Can be used with ~ 20pb-1

B tag efficiency measurement : System8 method Use of 3 uncorrelated taggers : J = b tagging algorithm we want to calibrate  B tagging efficiency in the system = εb(J) M = muon tagger (pTrel), B = presence of an opposite b tagged jet (enhance bbar events) Q(X,Y) fractions of jet that survive the X and Y tagger requirement in data εX efficiency for the X tagger (unknowns) Κ(X,Y) correlation between X and Y taggers (found in MC) 8 equations and 8 unknowns (εX , fb and fcl) = system fully constraint

System8 method results Advantages compared to the pTrel method : Reduce dependences in Monte Carlo Systematics clearly defined : error on correlation factors Κ(X,Y) Advantages compared to the pTrel method : Problems : Need more statistics than the pTrel method Still some problems at high jet pT (use of soft muon tagger pTrel ) Form CSC note

Mistag Rate Measurement: Negative Tag Method System

Test of Negative Tag Method in MC

Test Results of Negative Tag Method

Obtain Mistag Rate Matrix from Data

Test Results of Mistag Rate Matrix

Real Application in Background Estimation

Real Application in Background Estimation

Summary