W Charge Asymmetry at CDF

Slides:



Advertisements
Similar presentations
Regina Demina, University of Rochester 02/08/2012 Forward-backward asymmetry in top-antitop production in proton-antiproton collisions.
Advertisements

Chris Hays Duke University TEV4LHC Workshop Fermilab 2004 W Mass Measurement at the Tevatron CDF DØDØ.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
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
Heavy Flavor Production at the Tevatron Jennifer Pursley The Johns Hopkins University on behalf of the CDF and D0 Collaborations Beauty University.
University of Science & Technology of China (USTC) University of Science & Technology of China (USTC) W/Z+  ATLAS On behalf of ATLAS Collaboration.
Sung-Won Lee 1 Study of Jets Production Association with a Z boson in pp Collision at 7 and 8 TeV with the CMS Detector Kittikul Kovitanggoon Ph. D. Thesis.
Heavy charged gauge boson, W’, search at Hadron Colliders YuChul Yang (Kyungpook National University) (PPP9, NCU, Taiwan, June 04, 2011) June04, 2011,
W/Z PRODUCTION AND PROPERTIES Anton Kapliy (University of Chicago) on behalf of the ATLAS collaboration PHENO-2012.
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.
Unfolding jet multiplicity and leading jet p T spectra in jet production in association with W and Z Bosons Christos Lazaridis University of Wisconsin-Madison.
Gideon Bella Tel Aviv University On behalf of the ATLAS collaboration ATL-PHYS-PUB ATL-PHYS-PUB Prospects of measuring ZZ and WZ polarization.
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.
Direct di-  Tevatron On behalf of the & Collaborations Liang HAN University of Science & Technology of China (USTC)
Study of the to Dilepton Channel with the Total Transverse Energy Kinematic Variable Athens, April 17 th 2003 Victoria Giakoumopoulou University of Athens,
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)
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)
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.
Precision Measurements of W and Z Boson Production at the Tevatron Jonathan Hays Northwestern University On Behalf of the CDF and DØ Collaborations XIII.
1 EPS2003, Aachen Nikos Varelas ELECTROWEAK & HIGGS PHYSICS AT DØ Nikos Varelas University of Illinois at Chicago for the DØ Collaboration
LHCb: Xmas 2010 Tara Shears, On behalf of the LHCb group.
Emily Nurse W production and properties at CDF0. Emily Nurse W production and properties at CDF1 The electron and muon channels are used to measure W.
Alternatives: Beyond SUSY Searches in CMS Dimitri Bourilkov University of Florida For the CMS Collaboration SUSY06, June 2006, Irvine, CA, USA.
7/20/07Jiyeon Han (University of Rochester)1 d  /dy Distribution of Drell-Yan Dielectron Pairs at CDF in Run II Jiyeon Han (University of Rochester) For.
Jet Studies at CDF Anwar Ahmad Bhatti The Rockefeller University CDF Collaboration DIS03 St. Petersburg Russia April 24,2003 Inclusive Jet Cross Section.
Jet + Isolated Photon Triple Differential Cross Section Nikolay Skachkov: “Photon2007”, Paris, 9-13 July 2007 DO Measurement of Triple Differential Photon.
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.
October 2011 David Toback, Texas A&M University Research Topics Seminar1 David Toback Texas A&M University For the CDF Collaboration CIPANP, June 2012.
Don LincolnExperimental QCD and W/Z+Jet Results 1 Recent Dijet Measurements at DØ Don Lincoln Fermi National Accelerator Laboratory for the DØ Collaboration.
1 Measurement of the Mass of the Top Quark in Dilepton Channels at DØ Jeff Temple University of Arizona for the DØ collaboration DPF 2006.
A. Bertolin on behalf of the H1 and ZEUS collaborations Charm (and beauty) production in DIS at HERA (Sezione di Padova) Outline: HERA, H1 and ZEUS heavy.
April 7, 2008 DIS UCL1 Tevatron results Heidi Schellman for the D0 and CDF Collaborations.
Penny Kasper Fermilab Heavy Quarkonium Workshop 21 June Upsilon production DØ Penny Kasper Fermilab (DØ collaboration) 29 June 2006 Heavy Quarkonium.
Tomas Hreus, Pascal Vanlaer Overview: K0s correction stability tests Jet-pt correction closure test Study of Strangeness Production in Underlying Event.
RHIC-PV, April 27, 2007 M. Rijssenbeek 1 The Measurement of W ’s at the CERN and FNAL hadron colliders W ’s at RHIC ! W ’s at CERN – UA2 W ’s at FNAL -
Jet + Isolated Photon Triple Differential Cross Section Nikolay Skachkov: “Photon2007”, Paris, 9-13 July 2007 DO Measurement of Triple Differential Photon.
Stano Tokar, slide 1 Top into Dileptons Stano Tokar Comenius University, Bratislava With a kind permissison of the CDF top group Dec 2004 RTN Workshop.
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.
Upsilon production and μ-tagged jets in DØ Horst D. Wahl Florida State University (DØ collaboration) 29 April 2005 DIS April to 1 May 2005 Madison.
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.
1 Proton Structure Functions and HERA QCD Fit HERA+Experiments F 2 Charged Current+xF 3 HERA QCD Fit for the H1 and ZEUS Collaborations Andrew Mehta (Liverpool.
American Physical Society Meeting St. Louis, MO April th, 2008 Measuring the top mass at DØ using the Ideogram Method Amnon Harel
Joshua Moss (Ohio State University) on behalf of the ATLAS Collaboration ICHEP 2012, Melbourne 6 July 2012 ATLAS Electroweak measurements of W and Z properties.
The Top Quark at CDF Production & Decay Properties
PDFs from HERA to the LHC March 2005 A.M Cooper-Sarkar
Top mass measurements at the Tevatron
Top quark angular distribution results (LHC)
Forward-backward/charge asymmetry in top events
Precision measurements of electroweak parameters at the HL-LHC
Uncertainties on top quark mass due to modeling
Deep Inelastic Scattering 2006
Trang Hoang Florida State University - Dzero
Observation of Diffractively Produced W- and Z-Bosons
An Important thing to know.
Quarkonium production in ALICE
Di-jet production in gg collisions in OPAL
Investigation on QCD group
Electroweak Results from DØ
Constraints on PDF uncertainties from CDF
Study of e+e- pp process using initial state radiation with BaBar
W/Z and Di-Boson Results from ATLAS Srivas Prasad Harvard University On behalf of the ATLAS Collaboration Pheno Madison, Wisconsin May 09, 2011.
W/Z and Di-Boson Results from ATLAS Srivas Prasad Harvard University On behalf of the ATLAS Collaboration Pheno Madison, Wisconsin May 09, 2011.
Search for Narrow Resonance Decaying to Muon Pairs in 2.3 fb-1
Greg Heath University of Bristol
Observation of Diffractively Produced W- and Z-Bosons
Ronan McNulty University College Dublin
Measurement of the Single Top Production Cross Section at CDF
Susan Burke, University of Arizona
Measurement of b-jet Shapes at CDF
Presentation transcript:

W Charge Asymmetry at CDF Kevin McFarland University of Rochester on behalf of CDF collaboration Ph.D. thesis of Bo-Young Han DIS 2008, UC-London, 8 April 2008

K. McFarland, W Charge Asymmetry Outline Introduction and Analysis Technique Signal, Backgrounds and Corrections Uncertainties Preliminary results 8 April 2008 K. McFarland, W Charge Asymmetry

W Charge Asymmetry and PDFs At Tevatron, W± are produced primarily by uproton (danti-proton) and uanti-proton (dproton) W charge Asymmetry u d u quarks carry more momentum than d quarks 8 April 2008 K. McFarland, W Charge Asymmetry

Lepton Charge Asymmetry CDFII, 170 pb-1 Previous work from TeVatron has measured the charge asymmetry vs. lepton η in W→ℓν This observable is a convolution of the W charge asymmetry and V-A W decay angular distribution Lepton charge asymmetry W charge asymmetry 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Lepton and W Rapidity Lepton prefers to decay against boost 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Analysis Technique Measure W± rapidity Use W mass constraint solve eqn. answer : Weight the two solutions This method must be iterated to remove input bias shown it does not depend on assumed charge asymmetry can’t measure !!! Probability of angular distribution Differential W cross section 8 April 2008 K. McFarland, W Charge Asymmetry

Complications: Detector Effects true rapidity weighting factor response matrix Y1 Y2 wt1 wt2 YW YW FSR depends on physics input →should be iterated doesn’t depends on physics input →do not need to be iterated Response matrix to correct for detector acceptance, smearing and final state effects QED, W→τν→eννν 8 April 2008 K. McFarland, W Charge Asymmetry

Complications: W Production from the sea Sign of V-A angular bias flips when W± is produced from anti-quarks take this fraction as an input ratio of two angular distributions at each rapidity 8 April 2008 K. McFarland, W Charge Asymmetry

What is input, and what is measured? Inputs from theory: and Output from iteration: method documented in B.Y.Han et al., arXiv:hep-ph/0711.2859 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Outline Introduction and Analysis Technique Signal, Backgrounds and Corrections Uncertainties Preliminary results 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Summary of Data Issues Require one high ET electron and missing ET to tag the neutrino ETe>25(20) GeV in central (plug) detector missing ET>25 GeV Detector response, including missing ET, tuned on Z→e+e- sample Highlight backgrounds (primarily jets faking electrons) and charge mismeasurement also, trigger and detector acceptance and smearing 8 April 2008 K. McFarland, W Charge Asymmetry

Data and Simulation Kinematic Distributions Red : MC Blue : data Scale and resolution tuned on Z→e+e- 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Backgrounds Measure jet backgrounds directly in data use extra energy “isolation” around electron to separate, and fit shape to background fraction Illustrative fit (one of many) shown at right use jet sample to predict measured “yW” and charge from this sample uncertainty is ~0.15% of total sample A number of minor backgrounds (real Ws) from simulation electron 8 April 2008 K. McFarland, W Charge Asymmetry

Electron Charge Identification Charge identification is crucial for this measurement Forward tracking has fewer points at shorter lever arm Determine directly from (background subtracted) 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Outline Introduction and Analysis Technique Signal, Backgrounds and Corrections Uncertainties Preliminary results 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Systematic Effects Detector response energy scale and smearing for electron and recoil efficiency to find electron and pass missing ET cut Inputs PDF uncertainties (CTEQ6 PDF error sets) for total W production and quark/anti-quark fractions 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Evaluation Derive result with shifted parameters Systematics dominate only if yW<0.2 or >2.6 largest detector effect: energy scale largest PDF effect: qbar/q largest selection effect: elec. cuts charge fake rate uncertainty 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Outline Introduction and Analysis Technique Signal, Backgrounds and Corrections Uncertainties Preliminary results 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Uncertainties Unfolding correlates (strongly) the statistical errors in nearby bins Systematics also strongly correlated… PDF fitters, please exercise caution… 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Input PDFs We are in the process of documenting how result depends on input PDFs PDF fitters can explicitly put this in (or ignore if small) effect of increasing valence u+d by +5% effect of increasing sea u+d by +5% 8 April 2008 K. McFarland, W Charge Asymmetry

CDF Preliminary Result (1fb-1) Positive and negative yW agree, so fold Compare to NNLO (MRST) NLO error PDFs (CTEQ) 8 April 2008 K. McFarland, W Charge Asymmetry

CDF Preliminary Result (1fb-1) Compare CTEQ6M and MRST2006 with PDFs and their uncertainties 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Conclusions First direct measurement of W charge asymmetry despite additional complication of multiple solutions, it works! appears that it will have impact on d/u of proton Looking forward to working with PDF fitting groups to incorporate 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Outline Introduction and Analysis Technique Signal, Backgrounds and Corrections Uncertainties Preliminary results Backup 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Results 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Systematics 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Acceptance 8 April 2008 K. McFarland, W Charge Asymmetry

Plug Electron Tracking Efficiency 8 April 2008 K. McFarland, W Charge Asymmetry

QCD higher order corrections Our weight factor is initialized by one prediction. The parameterization of angular distribution : The ratio of anti-quark and quark in proton : Q(yW,PWT) using MC@NLO Differential cross-sections : dσ±/dyW KNNLO = (dσNNLO/dyW) / (dσLO/dyW) 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry f(PT) and g(PT) 8 April 2008 K. McFarland, W Charge Asymmetry

NNLO K-factor: (dσNNLO/dyW)/(dσLO/dyW) NNLO dσ±/dyW (mrst2002 PDFs) from theoretical prediction. 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry NNLO K-factor W charge asymmetry measurement using K-factor. 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Z PT at LO (Pythia) check if LO (Pythia) is tuned by DATA. Using Zee samples : zewk6d(Pythia) vs bhel0d(data) Looks MC agrees with data. 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry W Pt tune at MC@NLO Comparison of Pt distribution between NLO(Herwig) and LO(Pythia) Using W→eν samples Obtain the re-weight factor from the ratio of both We are going to re-weight the event of NLO. 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Q(yW,PWT) (cont.) 10 < PT and 10 < PT < 20 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Q(yW,PWT) (cont.) 20 < PT < 40 and 40 < PT < 60 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Q(yW,PWT) (cont.) 60 < PT < 80 and 80 < PT < 200 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Q factor + K-factor Even if QCD higher order correction makes small effect on the asymmetry, we believe that it describes better differential cross-section and angular distribution. 8 April 2008 K. McFarland, W Charge Asymmetry

K. McFarland, W Charge Asymmetry Q(yW,PWT) using MC@NLO W charge asymmetry measurement using NLO Q factor Compare it with previous result using LO Q factor 8 April 2008 K. McFarland, W Charge Asymmetry