Tevatron Results on W and Z Boson Production
|
|
- Andra Gibson
- 5 years ago
- Views:
Transcription
1 Les Arcs, Moriond QCD, March -9, 3 Tevatron Results on W and Z Boson Production Tommaso Dorigo (Università di Padova) Introduction to Run II New W/Z cross section results Cross section ratios and Γ W Dielectron asymmetry WW production Concluding remarks
2 Les Arcs, Moriond QCD, March -9, 3 Introduction to Run II at the Tevatron The Tevatron runs at s = 1.96 TeV since 1. So far L max = cm s 1. Total delivered luminosity: 18 pb 1. Expect to collect pb 1 in 3. The recycler will be integrated in data taking this summer. It will bring luminosity up by a factor. Other improvements are in progress. Tommaso Dorigo, Padova University
3 Les Arcs, Moriond QCD, March -9, 3 Tommaso Dorigo, Padova University 3
4 Les Arcs, Moriond QCD, March -9, 3 The new D and CDF II Since Run I both detectors have undergone massive improvements: CDF upgraded its silicon tracking (now 1+5+ layers), extended muon coverage to η < 1.5, and built a brand new plug calorimeter ( e ID up to η < ). D inserted an inner silicon tracker and a fiber tracker into a T axial field magnet. New mini-drift tubes for forward muons have been added; a new preshower improves electron triggering at low P T. Tommaso Dorigo, Padova University 4
5 Les Arcs, Moriond QCD, March -9, 3 W and Z production at the Tevatron W and Z bosons are produced at the Tevatron through q q ( ) annihilation. The cleanest signatures involve high-p T electrons and muons: W eν or µν, Z e + e or µ + µ ; the W τν decay can also be observed with clarity although backgrounds are larger. Other decays are hard to use for precise EW measurements ET Electron P T W W eν Muon Z P T P T P T U Hadronic recoil Underlying event Neutrino E T Z µ + µ U Hadronic recoil Underlying event Muon P T Tommaso Dorigo, Padova University 5
6 Les Arcs, Moriond QCD, March -9, 3 New σw measurements - 1: electrons W! e Cross Se 8 tion Analysis Blessing, EWK Meeting, 13 Feb 3 D and CDF presented 1.96 T ev cross sections last summer (ICHEP ). Ba kground FOR BLESSING: CDF updated its result adding data collected till Jan 3 (L = 7. ± 4.3 pb 1 ). Background sources: Sour es of the ba number out of ± (syst.); andidate events NQCD = 1344±8 (stat.) QCD pro esses stat 67sy st events W! (! e ) 768 ZN! (MC); We τ + e ν = 768 ± NZ e+ e = 344 ± 17 (MC); (from MC study) (from MC study) Number of the QCD ba from Start with central electron trigger (ET > 18 GeV ); 1.8 > 1 GeV /c; quality cuts on EHAD /EEM, Eiso, strip χ, E/P. 38, 68 W candidates; A = 4.6 ±.4(MC)±.69(syst)%. Tommaso Dorigo, Padova University vs. MET kground events was estimated plot, assuming that isolation and The QCD contamination is obtained NC E NB =N / by extrapolation Ninbg = the T vs A Ie plot: Isolation Fraction Iso MET are un /T > 5 GeV ; ET > 5 GeV, E PTe kground orrelated. Isolation vs. Missing Transverse Energy A C 1.6 CDF Run II Preliminary L ~ 7 pb 1.4 QCD Background C 1. 1 = B A.8.6 W e ν Candidates.4. B E T (GeV) 6
7 Les Arcs, Moriond QCD, March -9, 3 Acceptance systematics are dominated by: PDFs (.58%) Material (.9%) Total:.69%. Other factors: ǫ ID = 84. ±.7 ±.%; ǫ Zv = 95.1 ±.1 ±.5%; ǫ trig = 96.6 ±.1%. Events per GeV E T CDF Run II Preliminary, 7pb Cut Entries 9387 DATA Sum W eν MC Z ee MC W τν MC QCD E T, GeV Events per GeV/c CDF Run II Preliminary, 7pb Entries 3868 DATA Sum W eν MC Z ee MC W τν MC QCD M T, GeV/c Result: σ W B(W eν) =.64 ±.1 (stat.) ±.9 (syst.) ±.16(lum.) nb. ICHEP :.6 ±.7 ±.11 ±.6 nb (CDF),.67 ±.6 ±.33 ±.7 nb (D); Prediction by W.J.Stirling et al. (NNLO):.73 pb. Tommaso Dorigo, Padova University 7
8 Les Arcs, Moriond QCD, March -9, 3 New σ W measurements - : muons CDF updated its result for σ W B(W µν) with L = 7. ± 4.3 pb 1. CDF Run II Preliminary, 7pb Use central ( η <.6) muon triggers P T > GeV/c; E Iso ( R <.4) <.1 P T ; other fiduciality and matching cuts; remove cosmics, Z µµ; E/ T > GeV, 3 < M T < 1 GeV ; 1,599 W µν candidates Events per 3GeV/c DATA Entries 1599 Sum W µν MC 18 Z µµ MC W τν MC 16 QCD 14 Cosmic M T, GeV/c Tommaso Dorigo, Padova University 8
9 Les Arcs, Moriond QCD, March -9, 3 Tommaso Dorigo, Padova University 9
10 Les Arcs, Moriond QCD, March -9, 3 Backgrounds: Source Method Amount Cosmics Rev. z cut 1.8 ±.8 ±.9% QCD E/ T vs E Iso 1.3 ±.6 ±.6% Z µµ MC 5.31 ±.4 ±.% W τν MC 3. ±.14 ±.% Total 1.8 ±.18 ±.96% Events per 3GeV Data W µν MC CDF Run II Preliminary, 7pb Entries 1599 Acceptance: A = 14.8 ± 5 (stat) ±.51 (syst.)%; systematics mainly due to PDF (.41%), recoil scale (.3%); PDF contribution obtained by varying them to span ±1σ of dσ Z /dy measured in Run I; Recoil scale effect studied by shifting scale to get better agreement with MC and recomputing A. Result: σ W B(µν) =.64 ±. (stat.) ±.1 (syst.) ±.16 (lum) nb (CDF ICHEP :.7 ±.4 ±.19 ±.7 nb; D ICHEP :.67 ±.6 ±.33 ±.7 nb). Events per 3GeV Recoil E, GeV 5 CDF Run II Preliminary, 7pb Entries 6768 DATA Sum W µν MC Z µµ MC W τν MC QCD Cosmic E T, GeV Tommaso Dorigo, Padova University 1
11 Les Arcs, Moriond QCD, March -9, 3 σ W using τ leptons (CDF) Collect W τν signal with E/ T > 5 GeV L1 trigger, τ ID at L3. 1. Monojet events: E j T > 5 GeV, with one P T > 4.5 GeV track in 1 cone, no tracks in 1 3 ;. No other jet with E T > 5 GeV ; 3. E/ T > 5 GeV ; 4. tight electrons removed; 341 evts (611 ± 56 from bgr sources). Result: σ W B(τν) =.6 ±.7 ±.1 ±.16 nb. Using W eν signal removed at step (4), extract: R = B(τν)/B(eν) =.99 ±.3 (stat.) ±.4 (syst). 14 W τ ν : number of tracks, associated with the τ candidate CDF Run II Preliminary, 345 events number of tracks L = 7 pb Data W τ ν W µ ν W e ν Z τ τ QCD Tommaso Dorigo, Padova University 11
12 Les Arcs, Moriond QCD, March -9, 3 Z cross section: 1 - electrons (CDF) Data selection: Two central electrons E T > 5 GeV, P T > 1 GeV ; at least one must pass tight cuts; 66 < M ee < 116 GeV, opposite charge. 183 evts / 1 ± 5 from backgrounds. Other ingredients: Acceptance: 11.49±.6% (syst. mainly from material & PDF uncertainties); Z efficiency: 87. ±.9%, ǫ Zv = 95.1 ±.5%; Result: σ Z B(Z ee) = 67. ± 6.3 ± 15. ± 16. pb. (theory: 5.5 pb (Stirling, NNLO)). ÓÖ Ð Ò CDF Run II Preliminary L dt = 7.7 pb Ø Ï Ø ÓÖÖ Ø ÓÒ Z ee DATA Z ee MC Å ½½ λ ¾ Æ Ò ÇË Ë˵ ½ ¼ ¾¾µ Ø Øº µ Evts/ GeV/c E corr / P corr (GeV/c ) M ee Opposite Sign Z ee DATA Z ee MC CDF Run II Preliminary L dt = 7.7 pb Tommaso Dorigo, Padova University 1
13 Les Arcs, Moriond QCD, March -9, 3 Tommaso Dorigo, Padova University 13
14 Les Arcs, Moriond QCD, March -9, 3 Z cross section: - muons Both CDF and D have updated σ Z B(Z µµ). D: L = 31.8 pb 1 (Sept. to Jan. 3). two good muons, 1 isolated; P T > 15 GeV/c, R µµ >., E Iso(.5) <.5 GeV ; 1585 candidates, 1.5 ± 1.% backgrounds; Total acceptance:.163 ±.11. Result: σ Z B(µµ) = 63.8 ± 6.8 ± 17.3 ± 6.4 pb (ICHEP, electrons: 66 ± ± ± 1 pb) CDF: central µ, P T > GeV/c; 163 candidates N Z = 1618 ± 11. Result: σ Z B(µµ) = 46 ± 6 ± 1 ± 15 pb Events / 3 GeV Events per 1GeV/c D Run II Preliminary Data MC M µ+µ- (GeV) Entries 1631 Data Z µµ MC CDF Run II Preliminary, 7pb M µµ, GeV/c Tommaso Dorigo, Padova University 14
15 Les Arcs, Moriond QCD, March -9, 3 A global view of W/Z cross sections What do we expect to learn from these measurements? W/Z cross section measurements require critical understanding of detector and DAQ. Good to do it right from the start! Can use W yields to monitor acquired luminosity during the run and normalize other measurements involving electrons Ratios of cross sections tell us more σ W, Z B (pb) DØ and CDF Run Preliminary pp _ W+X lν+x pp _ Z+X ll+x DØ(e) Run DØ(µ) Run CDF(e) Run CDF(µ) Run DØ(e) DØ(µ) CDF(e) CDF(µ) UA1 UA 1 Center of Mass Energy (TeV) Tommaso Dorigo, Padova University 15
16 Les Arcs, Moriond QCD, March -9, 3 σ W /σ Z ratio and W width (CDF) Using the new W and Z cross section measurements CDF finds: R e = σ W B(W eν)/σ Z B(Z ee) = 9.88 ±.4 (stat.)±.47 (syst.), R µ = 1.69 ±.7 (stat.) ±.33 (syst.). (NNLO, Stirling: R th = 1.9). From WA values of W/Z widths and σ W /σ Z = ±.4 (Stirling, p.c.) we can then extract Γ W = σ W Γ W e Γ Z Γ e W Γ µ W σ Z Γ Z ee R : =.9 ±.6 (stat.)±.1 (syst.) GeV, =.11 ±.5 (stat.)±.7 (syst.) GeV (PDG:.118 ±.4 GeV ). The combined result is: Γ W =.146 ±.78 GeV Year World Average CDF II (e+µ) D I (e+µ) Standard Model CDF I (e) UA(e) UA1(e+µ) Γ(W) CDF Run II Preliminary L dt = 7. pb Tommaso Dorigo, Padova University 16
17 Mee_CCs_MC Mee_CCs_DT Entries Mean RMS Mee_CCs_DT Entries Mean 68.5 RMS Les Arcs, Moriond QCD, March -9, 3 A FB of electron pairs CDF used the new Run II data (5438 events) to measure A FB of e + e pairs from p p Z(γ )X e + e X, with 4 < M ee < 6 GeV. A FB (QCD) CDF Run II Preliminary (GeV) M ee χ /ndf = 18.4/15 Electron scale/resolution calibrated in data and MC in central and plug regions QCD bgr for CP combs is obtained from high-e iso electrons CDF Run II Preliminary CC Invariant Mass (GeV) CDF Run II Preliminary CP Invariant Mass (GeV) Points: data Yellow: Simulation CC Invariant Mass (M ee ) Same Sign CC Invariant Mass (M ee ) Same Sign (MC subtracted) For CC pairs, same-sign electrons N QCD = 1.5 ± 5.9 events; CP: N QCD = 18 ±65. Tommaso Dorigo, Padova University 17
18 Les Arcs, Moriond QCD, March -9, 3 Events/ GeV The new A FB measurement is corrected for acceptance, efficiency, resolution, and QED radiation. Results agree with Pythia predictions (GeV) M ee Points: Data Yellow:Simulation Green: Backgrounds CDF Run II Preliminary L=7pb A FB A FB CDF Run II Preliminary L=7pb - Z/γ* e e MC band includes several theoretical calculations -.4 Statistical Total M ee (GeV) CDF Run II Preliminary L=7pb - Z/γ* e e MC band includes several theoretical calculations Statistical Total M ee (GeV) + + Tommaso Dorigo, Padova University 18
19 Les Arcs, Moriond QCD, March -9, 3 Blessing Plots Searches for WW production φ(et,closest l,jet) In Run I CDF used 5 events (Nb = 1. ±.3) to measure σw W = ± 1.6 pb. A similar search for dilepton candidates is going on.5 in the sample used to look for dilepton tt production, 1.5 requiring Nj =. Total backgrounds amount to 1.5 ±.6 events, the 1 expected W W signal yield is.7 ±.6 events..5 Global likelihood So far events have been observed in L = 56 pb 1. 4 W + ud sample MC WW Data ee Data e µ Data µµ distribution( ont'd) ET (GeV) { CDF PRELIMINARY { WW! dilepton BG RUNI WW EVENTS MEAN RMS RUN I data WW BG Global Likelihood Tommaso Dorigo, Padova University 39 S/BG 5 1 S/ BG Number of events In the Run I sample an optimized search has been carried out for pp W W + X lνjj. Limits have been set at σw W < 61 pb. The search has established new methods to search for hadronic W jj decays, useful for Run II searches. Dave Waters Global likelihood cut -4-4 Global likelihood cut We set the G.L threshold at 1.5 to minimize the expe ted upper 19 limit of W +W produ tion.
20 Les Arcs, Moriond QCD, March -9, 3 Concluding remarks W and Z cross sections rise with s agrees well with NNLO; Z asymmetry probed up to s = 6 GeV ; other searches have started. Run II is starting to deliver - xs results already reached accuracy levels similar to Run I Next steps in EW physics are W mass, W asymmetry! We expect first results soon. Detectors largely understood with small caveats; not yet exploited to fullest potential Expect to collect at least pb 1 in 3; 3 pb 1 is stretch goal Tommaso Dorigo, Padova University
Electroweak Physics at the Tevatron
Electroweak Physics at the Tevatron Adam Lyon / Fermilab for the DØ and CDF collaborations 15 th Topical Conference on Hadron Collider Physics June 2004 Outline Importance Methodology Single Boson Measurements
More informationW and Z boson production in p p collisions from Run II of the Tevatron Collider
W and Z boson production in p p collisions from Run II of the Tevatron Collider P. Petroff To cite this version: P. Petroff. W and Z boson production in p p collisions from Run II of the Tevatron Collider.
More informationFirst V+jets results with CMS. Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8-10 Sep 2010, Durham
First V+jets results with CMS Vitaliano Ciulli (Univ. & INFN Firenze) V+jets workshop, 8- Sep 20, Durham Outline Jet and missing energy reconstruction W and Z selections and cross-section measurement First
More informationElectroweak results. Luca Lista. INFN - Napoli. LHC Physics
Electroweak results Luca Lista INFN - Napoli EWK processes at LHC p p W and Z production in pp collisions proceeds mainly form the scattering of a valence quark with a sea anti-quark The involved parton
More informationMeasurements of the W Boson Mass and Trilinear Gauge Boson Couplings at the Tevatron
Measurements of the Boson Mass and Trilinear Gauge Boson Couplings at the Tevatron John Ellison University of California, Riverside, USA Selection of and Z events Measurement of the mass Tests of the gauge
More informationFrom the TeVatron to the LHC UK HEP Forum, 7-8 May 2009 Emily Nurse
From the TeVatron to the LHC UK HEP Forum, 7-8 May 2009 0 σ(tt) M t single t helicity σ(/z) A (Y) Y Z M Jets Γ Z A FB di-bosons Z p T 1 This talk Craig Buttar σ(tt) M t single t helicity σ(/z) A (Y) Y
More informationPDF Studies at LHCb! Simone Bifani. On behalf of the LHCb collaboration. University of Birmingham (UK)
PDF Studies at LHCb! Simone Bifani University of Birmingham (UK) On behalf of the LHCb collaboration MENU 213 Rome 3th September - 4th October 213 Outline Introduction Analyses» Z/γ* ll, l =, e, τ#» W
More informationPrecise measurements of the W mass at the Tevatron and indirect constraints on the Higgs mass. Rencontres de Moriond QCD and High Energy Interactions
Precise measurements of the W mass at the evatron and indirect constraints on the Higgs mass Rafael Lopes de Sá for the CDF and DØ Collaborations March 11, 212 Rencontres de Moriond QCD and High Energy
More informationElectroweak Measurements at LHCb!
Electroweak Measurements at LHCb! Simone Bifani University of Birmingham (UK) on behalf of the LHCb collaboration LHCb workshop on quantum interference effects, QCD measurements and generator tuning CERN,
More informationZ boson studies at the ATLAS experiment at CERN. Giacomo Artoni Ph.D Thesis Project June 6, 2011
Z boson studies at the ATLAS experiment at CERN Giacomo Artoni Ph.D Thesis Project June 6, 2011 Outline Introduction to the LHC and ATLAS ((Very) Brief) Z boson history Measurement of σ Backgrounds Acceptances
More informationInclusive top pair production at Tevatron and LHC in electron/muon final states
Inclusive top pair production at Tevatron and LHC in electron/muon final states Andreas Jung for the ATLAS, CDF, CMS and D Collaboration Fermilab, DAB5 - MS 357, P.O. Box 5, Batavia, IL, 651, USA DOI:
More informationTOP AND ELECTROWEAK PHYSICS FROM THE TEVATRON
Physics in Collision - Zeuthen, Germany, June 26-28, 2003 TOP AND ELECTROWEAK PHYSICS FROM THE TEVATRON Mark C. Kruse (Representing the CDF and DØ collaborations) Duke University, Deparment of Physics,
More informationThe W-mass Measurement at CDF
2010-05 - 10 The W-mass Measurement at CDF Ilija Bizjak, University College London 1/33 Outline 1) Motivation for a W mass measurement Implications for the EW constraints on Higgs mass 2) Measurement of
More informationMeasurement of the W boson mass at Tevatron
Cracow Warsaw Workshop on LHC Faculty of Physics, University of Warsaw 26 March 2010 Measurement of the W boson mass at Tevatron Mikołaj Ćwiok University of Warsaw University of Warsaw Motivation for precise
More informationInclusive. W & Z measurements in CMS. Georgios Daskalakis. on behalf of CMS Collaboration. .C.S.R. Demokritos
Inclusive W & Z measurements in CMS Georgios Daskalakis.C.S.R. Demokritos on behalf of CMS Collaboration 1 Overview LHC hopefully will be proven to be a discovery machine but before that the measurement
More informationPhysics at Tevatron. Koji Sato KEK Theory Meeting 2005 Particle Physics Phenomenology March 3, Contents
Physics at Tevatron Contents Koji Sato KEK Theory Meeting 5 Particle Physics Phenomenology March 3, 5 mass measurement Top physics cross section Top mass measurement SM Higgs search Tevatron Run II Started
More informationWZ di-boson production at CMS
WZ di-boson production at CMS 1 Outline Physics motivations Existing results (Tevatron s = 1.96TeV) Existing prospects for CMS at s = 14TeV Preliminary prospects for CMS at s = 7TeV 2 WZ Physics motivation
More informationHiggs and Z τ + τ in CMS
Higgs and Z τ + τ in CMS Christian Veelken for the CMS Collaboration Moriond EWK Conference, March 14 th 2011 Z τ + τ - Production @ 7 TeV τ + Z τ - CMS Measurement of Z/γ* l + l -, l = e/µ: σ BR(Z/γ*
More informationP-P PHYSICS AT LHC. W and Z produc1on. Data and MC comparison. Lecture 4
P-P PHYSICS A LHC W and Z producon. Data and MC comparison Lecture 4 RIGGER URN ON rigger Efficiency 0.8 0.6 CMS preliminary, nb 8 67 y < 0.5 s = 7 ev 0 0.4 0. 0 MinBias Jet6u Jet5u Jet0u Anti-k R=0.5
More informationHiggs-related SM Measurements at ATLAS
Higgs-related SM Measurements at ATLAS Junjie Zhu University of Michigan 2 nd MCTP Spring Symposium on Higgs Boson Physics Outline Introduction Isolated γγ cross section (37 pb -1, Phys. Rev. D 85, 012003
More informationPhysics at Hadron Colliders
Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD
More informationATLAS-CONF October 15, 2010
ATLAS-CONF-2010-096 October 15, 2010 Data-driven background estimation for the H τ + τ τ h search at 7 TeV with the ATLAS detector Ian Howley 7 December 2010 1 Motivation One of the primary LHC physics
More informationPhysics with Tau Lepton Final States in ATLAS. Felix Friedrich on behalf of the ATLAS Collaboration
Physics with Tau Lepton Final States in ATLAS on behalf of the ATLAS Collaboration HEP 2012, Valparaiso (Chile), 06.01.2012 The Tau Lepton m τ = 1.8 GeV, heaviest lepton cτ = 87 μm, short lifetime hadronic
More informationMeasurement of the Z ττ cross-section in the semileptonic channel in pp collisions at s = 7 TeV with the ATLAS detector
Measurement of the Z ττ cross-section in the semileptonic channel in pp collisions at s = 7 TeV with the ATLAS detector Sofia Consonni Università di Milano & INFN XCVII Congresso Nazionale della Società
More informationTop and Electroweak Physics at. the Tevatron
Top and Electroweak Physics at 1 the Tevatron Graham W. Wilson University of Kansas for the CDF and DØ Collaborations April APS 2008, St. Louis, MO. April 12 th 2008 Introduction Top Physics Overview Cross-section
More informationMeasurements of the tt Cross Section and Top Mass at CDF
Measurements of the tt Cross Section and Top Mass at University of Chicago / LBNL For the Collaboration HCP 2004, 06/15/04, p. 1 Studying the tt Cross Section Main question: is top quark adequately described
More informationCDF top quark " $ )(! # % & '
$% CDF quark 7 3 5 ( "#! Tevatron Run II Started Spring 1. proton-antiproton collider with (Run I :. antiproton recycler commissioning electron cooling operational by Summer 5. increase in luminosity.
More informationSearches for Strong Dynamics at the TEVATRON
Searches for Strong Dynamics at the TEVATRON Hereafter I Present Preliminary Results on Behalf of the CDF and D0 Collaborations OUTLINE I. Introduction II. Search for Excited Electrons III. Search for
More informationSearch for ZZ production in the 4 lepton channel with 4.8 fb 1 of data
Search for ZZ production in the 4 lepton channel with 4.8 fb 1 of data M. Bauce INFN and University of Padova CDF Italia 1-2 September 29 M. Bauce (INFN Padova) ZZ llll cross-section CDF Italia 1-2/9/9
More informationAtlas Status and Perspectives
Atlas Status and Perspectives Bruno Mansoulié (IRFU-Saclay) On behalf of the Topics The hot news: Heavy Ion analysis Data taking in 2010 Luminosity, Data taking & quality, trigger Detector performance
More informationRecent Heavy Flavors results from Tevatron. Aleksei Popov (Institute for High Energy Physics, Protvino) on behalf of the CDF and DØ Collaborations
Recent Heavy Flavors results from Tevatron Aleksei Popov (Institute for High Energy Physics, Protvino) on behalf of the CDF and DØ Collaborations March 27, 2017 Outline Tevatron, CDF and DØ Confirmation
More informationThe Tevatron s Search for High Mass Higgs Bosons
The Tevatron s Search for High Mass Higgs Bosons Konstantinos A. Petridis University of Manchester On behalf of the CDF and DØ Collaborations K.A. Petridis (University of Manchester) Tevatron High Mass
More informationRecent Results on New Phenomena and Higgs Searches at DZERO
Recent Results on New Phenomena and Higgs Searches at DZERO Neeti Parashar Louisiana Tech University Ruston, Louisiana U.S.A. 1 Outline Motivation for DØ Run II Detector at Fermilab The Fermilab Tevatron
More informationDirect Measurement of the W Total Decay Width at DØ. Outline
Direct Measurement of the W Total Decay Width at DØ Introduction Junjie Zhu University of Maryland On behalf of the DØ Collaboration Monte Carlo Simulation Event Selection Outline Determination of the
More informationSearch for Charginos and Neutralinos with the DØ Detector
SUSY 006, 06/3/006 Marc Hohlfeld Search for Charginos and Neutralinos with the DØ Detector Marc Hohlfeld Laboratoire de l Accélérateur Linéaire, Orsay on behalf of the DØ Collaboration SUSY 006, 06/3/006
More informationPoS(DIS 2010)190. Diboson production at CMS
(on behalf of the CMS collaboration) INFN-Napoli & University of Basilicata E-mail: fabozzi@na.infn.it We present an analysis strategy based on Monte Carlo simulations for measuring the WW and WZ production
More informationSearching for Supersymmetry at the LHC David Stuart, University of California, Santa Barbara. CMS SUSY Search, D. Stuart, June 2011, Lisbon!
Searching for Supersymmetry at the LHC David Stuart, University of California, Santa Barbara CMS SUSY Search, D. Stuart, June 2011, Lisbon! 1! Searching for Supersymmetry at the LHC David Stuart, University
More informationtop quark mass measurements
top quark mass measurements Ulrich Heintz 11/8/006 DESY seminar - Ulrich Heintz 1 outline the top quark the top quark factory top quark production and decay top quark mass in the lepton+jets channel top
More informationOliver Stelzer-Chilton University of Oxford High Energy Physics Seminar Michigan State University
First Run II Measurement of the W Boson Mass by CDF Oliver Stelzer-Chilton University of Oxford High Energy Physics Seminar Michigan State University April 3 rd, 2007 1. Motivation Outline 2. W Production
More informationDilepton Forward-Backward Asymmetry and electroweak mixing angle at ATLAS and CMS
Dilepton Forward-Backward Asymmetry and electroweak mixing angle at ATLAS and CMS University of Rochester E-mail: jyhan@fnal.gov We present measurements of the forward-backward asymmetry in Drell-Yan dilepton
More informationDirect measurement of the W boson production charge asymmetry at CDF
Direct measurement of the boson production charge asymmetry at CDF Eva Halkiadakis Rutgers University For the CDF collaboration Joint Experimental-Theoretical Physics Seminar Fermilab May 22 2009 Outline
More informationSEARCH FOR 4 TH GENERATION QUARKS AT CMS
SEARCH FOR 4 TH GENERATION QUARKS AT CMS Kai-Feng Chen National Taiwan University LHC symposium in PSROC annual meeting January 6 th 0, National Normal University, Taipei 4TH GENERATIONS: WHY? WHY NOT?
More informationHighlights of top quark measurements in hadronic final states at ATLAS
Highlights of top quark measurements in hadronic final states at ATLAS Serena Palazzo 1,2,, on behalf of the ATLAS Collaboration 1 Università della Calabria 2 INFN Cosenza Abstract. Measurements of inclusive
More informationMeasurement of Properties of Electroweak Bosons with the DØ Detector
Measurement of Properties of Electroweak Bosons with the DØ Detector Laboratoire de Physique Subatomique et de Cosmologie, 53, rue des Martyrs, 38026, Grenoble Cedex, France. E-mail: Hengne.Li@in2p3.fr
More informationFrom Precision Electro-weak Physics to Beyond-the-SM Physics Searches
From Precision Electro-weak Physics to Beyond-the-SM Physics Searches PING TAN Oct. 22, 2012 Outline W charge asymmetry analysis Search for BSM physics with 2leptons +2jets Precision Electro-weak Physics
More informationW/Z Production Cross Sections and Asymmetries at ECM = 2TeV
W/Z Production Cross Sections and Asymmetries at ECM = 2TeV Dr. Angela Bellavance (University of Nebraska for the CDF and DØ collaborations ) Motivation Experiments and Detectors Z and W Cross Sections
More informationTop production at the Tevatron
Top production at the Tevatron Bob Hirosky University of Virginia for the CDF and D0 Collaborations Moriond Moriond QCD 2017 1 Top production at the Tevatron Top mass from differential cross section Polarization
More informationW, Z and top production measurements at LHCb
1 W, Z and top production measurements at LHCb Lorenzo Sestini, on behalf of the LHCb collaboration. Universitá di Padova e INFN E-mail: lorenzo.sestini@cern.ch The LHCb experiment offers a complementary
More informationProton anti proton collisions at 1.96 TeV currently highest centre of mass energy
Tevatron & Experiments 2 Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy Tevatron performing very well 6.5 fb 1 delivered (per experiment) 2 fb 1 recorded in 2008 alone
More informationQCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration
QCD at CDF Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration Jet Inclusive Cross-Section Underlying event studies Jet Shapes Specific processes _ W+Jets, γ + γ, γ + b/c, b-jet / bb jet Diffraction
More informationTop Physics. Claudio Campagnari University of California Santa Barbara
Top Physics Claudio Campagnari University of California Santa Barbara 1 Outline Top quark introduction What is interesting about top physics (brief) Top Physics program as CMS Emphasis on startup, status
More informationSingle-Top at the Tevatron
Single-Top at the Tevatron Bernd Stelzer University of Toronto on behalf of the CDF and DØD Collaborations 15 th International Conference on Hadron Collider Physics, Michigan State University, 14-18 June
More information2 ATLAS operations and data taking
The ATLAS experiment: status report and recent results Ludovico Pontecorvo INFN - Roma and CERN on behalf of the ATLAS Collaboration 1 Introduction The ATLAS experiment was designed to explore a broad
More informationIntroduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production.
Introduction. The LHC environment. What do we expect to do first? W/Z production (L 1-10 pb -1 ). W/Z + jets, multi-boson production. Top production. Early discoveries? Conclusions. 2 First collisions
More informationPHYS 5326 Lecture #23
PHYS 5326 Lecture #23 Monday, Apr. 21, 2003 Dr. Backgrounds to Higgs Searches Requirement on Experiments for Higgs Searches 1 Announcement Semester project presentation 1:00 4:00pm, Wednesday, May 7 in
More informationMeasurement of W and Z boson cross sections in pp collisions at 7 TeV with the ATLAS detector
Measurement of W and Z boson cross sections in pp collisions at 7 ev with the ALAS detector Ryan Reece University of Pennsylvania On behalf of the ALAS Collaboration [1] photo: naotakem he International
More informationHiggs cross-sections
Ph.D. Detailed Research Project Search for a Standard Model Higgs boson in the H ZZ ( ) 4l decay channel at the ATLAS Experiment at Cern Ph.D. Candidate: Giacomo Artoni Supervisor: Prof. Carlo Dionisi,
More informationMeasurement of the Higgs Couplings by Means of an Exclusive Analysis of its Diphoton decay
Measurement of the Higgs Couplings by Means of an Exclusive Analysis of its Diphoton decay i.e. what do we know about the Higgs Marco Grassi The Discovery of a New Boson Evidence of a new boson with 5
More informationSearch for SUSY at CMS in lepton or photon final states. PANIC 2011 K. Theofilatos (on behalf of CMS)
Search for SUSY at CMS in lepton or photon final states CMS in one slide Optimal design for reconstructing leptons & photons Compact & precisely aligned detector with B=3.8 T Calorimeters operating inside
More informationMeasurement of the W-mass with the ATLAS detector
Measurement of the W-mass with the ALAS detector Oleh Kivernyk CEA/Irfu/SPP July, 0 Oleh Kivernyk (CEA/Irfu/SPP) Measurement of the W-mass with the ALAS detector July, 0 / Motivation Relation between M
More informationEW Physics at LHC. phi= mu_4: pt=7.9 GeV, eta=-1.13, phi=0.94. Toni Baroncelli:
EW Physics at LHC Event display of a 2e2mu candidate. EventNumber: 12611816 RunNumber: 205113 m_4l=123.9 GeV. m_12=87.9 GeV, m_34=19.6 GeV. e_1: pt=18.7 GeV, eta=-2.45, phi=1.68,. 15/09/17 e_2: pt=75.96
More informationPrecision Electroweak Measurements at the Tevatron
Precision Electroweak Measurements at the Tevatron The W mass @ Tevatron Effec9ve weak mixing angle The Top Mass @ Tevatron Iain Bertram, Lancaster University for the D0 Collabora9on DIS 2017-6 April 2017
More informationMeasurement of the Inclusive Isolated Prompt Photon Cross Section at CDF
of the Inclusive Isolated Cross at IFAE Barcelona HEP Seminar University of Virginia Outline Theoretical introduction Prompt photon production The The Photon detection prediction The pqcd NLO prediction
More informationInclusive SUSY Searches at CMS with Emphasis on Detector Systematics
Inclusive SUSY Searches at with Emphasis on Detector Systematics R. Cavanaugh (on behalf of ) University of Florida SUSY06 Detector Background Calibrations Inclusive Search Strategies Detector Systematics
More informationTop quark mass at ATLAS and CMS
Top quark mass at ATLAS and CMS (Introduction) Direct measurements Template/Ideogram based Indirect measurements Unfolded shapes/cross sections Conclusions & Outlook Andreas Jung for the ATLAS & CMS collaboration
More informationin Section The H ZZ 4l channel
14 Events / 2 GeV Events - Fitted bkg 10000 8000 6000 4000 2000 500 400 300 200 100 0-100 -200 ATLAS -1 s = 7 TeV Ldt = 4.8 fb -1 s = 8 TeV Ldt = 20.7 fb Data 2011+2012 SM Higgs boson m =126.8 GeV (fit)
More informationTop production measurements using the ATLAS detector at the LHC
Top production measurements using the ATLAS detector at the LHC INFN, Sezione di Bologna and University of Bologna E-mail: romano@bo.infn.it This paper is an overview of recent results on top-quark production
More informationSearch for a heavy gauge boson W e
Search for a heavy gauge boson W e Cornell University LEPP Journal Club Seminar April 1, 2011 The LHC Machine 2 The beginning of the LHC era First collisions at 7 TeV confirmed on March 30, 2010 There
More informationSearch for High Mass SM Higgs at the Tevatron
Search for High Mass SM Higgs at the Tevatron Les Rencontres de Physique de la Vallee D'Aoste Mar. 6, 2009 Herbert Greenlee Fermilab for the CDF and D0 Collaborations SM Higgs Boson Direct Limit (LEP)
More informationSearches for New Phenomena in Events with Multiple Leptons with the ATLAS Detector
Searches for New Phenomena in Events with Multiple Leptons with the ALAS Detector ÜLİN VAROL University of Massachusetts, Amherst On Behalf of the ALAS Collaboration OULINE Introduction Excited e/μ Search
More informationFirst studies towards top-quark pair. dilepton channel at s = 13 TeV with the CMS detector
First studies towards topquark pair differential cross section measurement in the dilepton channel at s = 13 TeV with the CMS detector Mykola Savitskyi, Maria Aldaya, Carmen Diez Pardos et al. DESYCMS
More informationMeasurement of the mass of the W boson at DØ
Measurement of the mass of the W boson at DØ 1 IPNL, Université de Lyon, Université Lyon 1, CNRS/IN2P3 4 Rue E. Fermi 69622 Villeurbanne, France E-mail: kurca@in2p3.fr We present a measurement of the mass
More informationTop Physics in Hadron Collisions
Top Physics in Hadron Collisions Dirk Dammann DESY 2010-02-04 1 / 44 Outline 1 2 3 4 2 / 44 Outline Motivation Top Production Top Decay Top Physics 1 Motivation Top Production Top Decay Top Physics 2 3
More informationEarly Physics with the CMS detector at LHC
Early Physics with the CMS detector at LHC HLPW2008 6. 8. March 2008 Spa, Belgium Andre Holzner CERN/CMS Outline Status and schedule CMS LHC Early data analyses: The roadmap to discovering new physics
More informationSearch for Resonant Slepton Production with the DØ-Experiment
Overview Search for Resonant Slepton Production with the DØ-Experiment Christian Autermann, III. Phys. Inst. A R-parity violating Supersymmetry Resonant Slepton Production and Neutralino Decay Data selection
More informationPoS(EPS-HEP2011)250. Search for Higgs to WW (lνlν, lνqq) with the ATLAS Detector. Jonas Strandberg
with the ATLAS Detector Royal Institute of Technology, KTH, Stockholm, Sweden E-mail: jostran@kth.se Higgs boson searches in the H WW ( ) lνlν (l = e, µ) and the H WW ( ) lνqq decay modes, using. fb of
More informationPrecision QCD at the Tevatron. Markus Wobisch, Fermilab for the CDF and DØ Collaborations
Precision QCD at the Tevatron Markus Wobisch, Fermilab for the CDF and DØ Collaborations Fermilab Tevatron - Run II Chicago Ecm: 1.8 1.96 TeV more Bunches 6 36 Bunch Crossing 3500 396ns CDF Booster Tevatron
More informationTevatron Physics Prospects. Paul Grannis, for the CDF and DØ collaborations ICFA Seminar, Oct
Tevatron Physics Prospects Paul Grannis, for the CDF and DØ collaborations ICFA Seminar, Oct. 29 2008 CDF and DØ Operations Fermilab is planning to run CDF and DØ through FY2010. The Tevatron is now delivering
More informationPerformance of muon and tau identification at ATLAS
ATL-PHYS-PROC-22-3 22/2/22 Performance of muon and tau identification at ATLAS On behalf of the ATLAS Collaboration University of Oregon E-mail: mansoora.shamim@cern.ch Charged leptons play an important
More informationProspects for Higgs Searches at CDF in Run II
Prospects for Higgs Searches at CDF in Run II DPF2000 Columbus, Ohio August 9-12, 2000 Richard E. Hughes Department of Physics The Ohio State University Acknowledgements: Report of the Tevatron Higgs Working
More informationTop Physics at CMS. Intae Yu. Sungkyunkwan University (SKKU), Korea Yonsei University, Sep 12 th, 2013
Top Physics at CMS Intae Yu Sungkyunkwan University (SKKU), Korea Seminar @ Yonsei University, Sep 12 th, 2013 Outline Overview of CMS Operation Korea CMS Group Doing Top Physics at LHC Top Production
More informationThe Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS CR -2013/016 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 18 January 2013 (v2, 21 January 2013)
More informationHighlights of top-quark measurements in hadronic nal states at ATLAS
Highlights of top-quark measurements in hadronic nal states at ATLAS Serena Palazzo on behalf of the ATLAS collaboration XLVII International Symposium on Multiparticle Dynamics Tlaxcala, Mexico September
More informationPoS(EPS-HEP 2013)215. WW, WZ, and ZZ production at CMS. Jordi DUARTE CAMPDERROS (on behalf of CMS collaboration)
(on behalf of CMS collaboration) Universidad de Cantabria/CSIC E-mail: jorge.duarte.campderros@cern.ch We present the WW, WZ and ZZ production cross sections measurements and constraints on anomalous triple-gauge
More informationB-quark discovery. e+ e- PETRA GeV TRISTAN 61.4 GeV LEP Mz Mt > 45.8 GeV
1970s B-quark discovery e+ e- PETRA 12-47 GeV TRISTAN 61.4 GeV LEP Mz Mt > 45.8 GeV p+p- ISR 60 GeV SppS 630 GeV Tevatron 1800 GeV 1984 UA1 Mt = 40 ± 10 1989 UA1 Mt > 60 GeV UA2 Mt > 69 GeV 1989 CDF Mt
More informationMeasurement of the Z to tau tau cross section with the ATLAS detector
Measurement of the Z to tau tau cross section with the ALAS detector On behalf of the ALAS Collaboration Charles University in Prague, Faculty of Mathematics and Physics, Institute of Particle and Nuclear
More informationDon Lincoln. QCD Results from the Tevatron
Recent Don Lincoln Fermilab DØ Calorimeter Uranium-Liquid Argon Calorimeter stable, uniform response, radiation hard Compensating: e/π 1 Uniform hermetic coverage η 4.2, recall η ln[tan(θ/2)] Longitudinal
More informationMuon reconstruction performance in ATLAS at Run-2
2 Muon reconstruction performance in ATLAS at Run-2 Hannah Herde on behalf of the ATLAS Collaboration Brandeis University (US) E-mail: hannah.herde@cern.ch ATL-PHYS-PROC-205-2 5 October 205 The ATLAS muon
More informationTobias Golling - SCIPP - August 24th 2004
Measurement of the Top Quark Pair Production Cross Section using a Topological Likelihood and using Lifetime b-tagging with the DØ Detector in Run II at the Fermilab Tevatron at a center of mass energy
More informationPhysics at Hadron Colliders Part II
Physics at Hadron Colliders Part II Marina Cobal Università di Udine 1 The structure of an event One incoming parton from each of the protons enters the hard process, where then a number of outgoing particles
More informationMeasurement of the Muon Charge Asymmetry in Inclusive pp W (μν) + X Production at s = 7 TeV. Saranya Ghosh (EHEP, TIFR) India-CMS meeting
Measurement of the Muon Charge Asymmetry in Inclusive pp W (μν) + X Production at s = 7 TeV Saranya Ghosh (EHEP, TIFR) India-CMS meeting 18th December, 2012 Contents Introduction Datasets Details of analysis
More informationHigh-pT lepton final states at 13 TeV (W and Z searches)
High-pT lepton final states at TeV (W and Z searches) James Catmore (University of Oslo, Norway) on behalf of the ATLAS and CMS Collaborations 5st Rencontres de Moriond EW 06 W and Z Many BSM models predict
More informationStandard Model physics with taus in ATLAS
Standard Model physics with taus in ATLAS IFJ PAN, Cracow, Poland Why we are interested in taus? Tau leptons play an important role in the physics program of the ATLAS experiment as they are tools in many
More informationQCD Measurements at DØ
QCD Measurements at DØ University of Texas -Arlington- Seminar, University of Virginia January 24th 27 TeVatron Collider at Fermilab Proton-Antiproton Collisions at Center-of-Mass s = 1.96 TeV Two Multi-Purpose
More informationMeasurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron
Measurements of the Masses, Mixing, and Lifetimes, of B Hadrons at the Tevatron Mike Strauss The University of Oklahoma The Oklahoma Center for High Energy Physics for the CDF and DØ Collaborations Outline
More informationRecent Results on Top Physics at CMS
Recent Results on Top Physics at CMS Jasmin Gruschke (KIT) on behalf of the CMS Collaboration Moriond/QCD: Rencontres de Moriond on QCD and High Energy Interactions March 2 th -29 th 211 Jasmin.Gruschke@cern.ch
More informationNEWS FROM THE TOP. 1. Pair Production of Top Quarks Cross Section Search for Resonances Forward-Backward Asymmetry
NEWS FROM THE TOP Results from CDF and D0 on: 1. Pair Production of Top Quarks Cross Section Search for Resonances Forward-Backward Asymmetry 2. Single Top Production Search for SM EWK Production Search
More informationLa ricerca dell Higgs Standard Model a CDF
La ricerca dell Higgs Standard Model a CDF Melisa Rossi INFN-TS Giornata di seminari INFN Trieste - 7 Luglio 2009 FNAL: Fermi National Accelerator Lab Tevatron currently provides the highest energy proton-antiproton
More informationPoS(CORFU2016)060. First Results on Higgs to WW at s=13 TeV with CMS detector
First Results on Higgs to WW at s=13 ev with CMS detector Università di Siena and INFN Firenze E-mail: russo@fi.infn.it he first measurement of the Higgs boson cross section at 13 ev in H WW 2l2ν decay
More informationInvariant Mass, Missing Mass, jet reconstruction and jet flavour tagging
1 Experimentelle Methods of Particle Physics HS 215 http://www.physik.uzh.ch/lectures/empp/ Wednesday 16.12.15 and Thursday 17.12.15 Invariant Mass, Missing Mass, jet reconstruction and jet flavour tagging
More information