Top Quark Production at the LHC. Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations

Size: px
Start display at page:

Download "Top Quark Production at the LHC. Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations"

Transcription

1 Top Quark Production at the LHC Masato Aoki (Nagoya University, Japan) For the ATLAS, CMS Collaborations

2 Phys. Rev. D 83 (2011) , Phys. Rev. D 82 (2010) , Phys. Rev. D 81 (2010) , Comput. Phys. Commun. 182 (2011) 1034 LHC: top quark factory with pp collisions s 7 TeV 8 TeV Top pair Single top: t-ch Single top: s-ch ± ± 0. 2 Single top: Wt ± ± fb TeV + 20 fb TeV per experiment 5,600,000 top pairs, 2,700,000 single top events Top Quark Production at the LHC 2

3 Measurement of top quark Precise tests of perturbative QCD Precise understanding of background in new physics and Higgs searches New physics may be associated with top quark production Top Quark Production at the LHC 3 t H H t t c,g t c,g t t W W t t

4 Inclusive σ tt σ 7 TeV pp collisions ATLAS and CMS combination Total uncertainty : 5.8% ATLAS-CONF CMS PAS TOP First LHC combination First step in the discussion towards the harmonization of systematic treatment For the moment there were still important differences: e.g. treatment of generator systematics This could be a very good motivation for top modeling studies Top Quark Production at the LHC 4

5 New results on inclusive σ tt Improved analysis technique CMS: dilepton with 2.3 fb ± 2. 5 stat syst ± 3. 6 lumi pb More refined event selections and analysis techniques, better estimate of systematics Eur. Phys. J. C72 (2012) 2202 σ tt New tool ATLAS: l+jets with 2.8 fb ± 2 stat ± 17 syst ± 3 lumi pb Soft Muon b-tagger ATLAS-CONF BSM-sensitive channel ATLAS: t+jets with 1.7 fb -1 Use hadronic tau 194 ± 18 stat ± 46 syst pb Eur. Phys. J. C, 73 3 (2013) 2328 CMS: t+jets with 3.9 fb -1 Use hadronic tau 152 ± 12 stat ± 32 syst ± 3 lumi pb arxiv: Energy: 8 TeV ATLAS: l+jets with 5.8 fb ± 2 stat ± 31 syst ± 9 lumi pb CMS: l+jets with 2.8 fb ± 9 stat syst ± 10 lumi pb CMS: dilepton with 2.4 fb ± 3 stat ± 11 syst ± 10 lumi pb ATLAS-CONF , CMS PAS TOP , CMS PAS TOP Top Quark Production at the LHC 5

6 Eur. Phys. J. C (2013) 73: 2261 tt differential cross 7 TeV, 2.05 fb -1, l+jets, at least one b-tag tt reconstruction by likelihood-based kinematic fitter Robust unregularized unfolding of m tt, y tt, p T tt compared with MCFM, ALPGEN, MC@NLO (and approx. NNLO for m tt ) Mostly systematics dominated (Jet/E T miss reco.): 10~20% Full covariance matrix provided All the measurements are in agreement with the standard model Top Quark Production at the LHC 6

7 arxiv: , CMS PAS TOP , CMS PAS TOP tt differential cross 7 TeV 5 fb -1, and 8 TeV 12 fb -1 l+jets channel (at least 4 jets, at least 2 b-tagged jets) tt reconstruction: Constrained kinematic fitting algorithm Typical systematic uncertainty: 5.4% 3.9% from experimental uncertainty 3.8% from modeling uncertainty Dilepton channel (at least 2 jets, at least 1 b-tagged jets) tt reconstruction: Alternative kinematic reconstruction method Wider top-mass assumption (100GeV - 300GeV ) Typical systematics uncertainty: 3.9% 2.8% from experimental uncertainty 2.7% from modeling uncertainty Top Quark Production at the LHC 7

8 arxiv: , CMS PAS TOP , CMS PAS TOP tt differential cross 7 TeV data 8 TeV data Good agreement between data and theoretical predictions The approximate NNLO provides the best description of the data Top Quark Production at the LHC 8

9 ATLAS-CONF Jet multiplicity in tt event ATLAS: 7 TeV, 4.7fb -1, l+jets channel, at least one b-tagged jet Number of jets (n jets ) measurement varying jet p T threshold Unfolded n jets distributions compared with several MC predictions Systematics dominated by Jet/E T miss reco. Discrepancy at large n jets for MC@NLO+HERWIG Reasonable agreement with ALPGEN+PYTHIA(or HERWIG) and POWHEG+PYTHIA p T >25GeV p T >40GeV p T >60GeV Top Quark Production at the LHC 9

10 CMS PAS TOP Additional jets in l+jets CMS: 7 TeV, 5 fb -1, l+jets channel Additional jets in tt events extracted by fitting to likelihood discriminant Comparing with MadGraph, MC@NLO, POWHEG A slight discrepancy with MC@NLO Top Quark Production at the LHC 10

11 Eur.Phys.J. C72 (2012) 2043, CMS PAS TOP Additional jets in dilepton Look at tt (ll + 2 b-jets) + additional jets ATLAS: 2 fb 7TeV CMS: 5 fb TeV Gap fraction: Fraction of events produced in the absence of an additional jet above a p T (Q 0 ) threshold Full rapidity interval: All those generators give a reasonable description of the data Central: MC@NLO is too large Forward: None of the predictions agrees with data Central y 2.4 y 2.1 Forward Top Quark Production at the LHC 11

12 CMS PAS TOP CMS: bb associated with tt 7 TeV, 5 fb -1 Dilepton + 4 jets Measure σ(tt bb)/σ(tt jj) Large cancellation of uncertainties b ID by Combined Secondary Vertex tagger (CSV) Combining SV and Track-based lifetime info Signal extraction by fitting to b-jet multiplicity σ(tt bb)/σ tt jj = 3. 6 ± 1. 1 stat ± 0. 9(syst) MADGRAPH: 1.2% POWHEG: 1.3% Δ = 39% 31%: Data stat. 23%: mistag rate 6.7%: Signal modeling 6.0%: b-tag eff. Top Quark Production at the LHC 12

13 Single top at LHC Alternative top quark production via the weak interaction Sensitive to many models of new physics Allow for a measure of V tb without assumptions about the number of quark generations Can be used to measure the b-quark parton distribution function t-channel s-channel Wt-channel Top Quark Production at the LHC 13

14 Phys. Lett. B 716 (2012) , Phys. Rev. Lett. 110 (2013) Wt associated TeV Final state: two leptons + E miss T + one b-jet Simultaneous fit of BDT outputs in different jet-bin regions (1-jet bin: signal region, 2>=jet bin: background control region) First evidence from ATLAS using 2fb -1, and confirmation by CMS with more stats. Δσ/σ=34% 16%: JES 15%: PS 10%: Gen. 10% Pile-up Δσ/σ=31% 20%: Stat. 15%: JES 10%: PS 22 variables 4 variables L [fb -1 ] Wt cross section [pb] Significance V tb ATLAS ± 2. 9(stat.) ± 4. 9(syst.) 3.3σ CMS σ exp (th.) Top Quark Production at the LHC 14

15 CMS PAS TOP , ATLAS-CONF t-channel single TeV miss Final state: one lepton + E T + one b-jet + one recoil jet Signal extracted by a fitting with ATLAS: NN discriminant CMS: η distribution of recoil jet * 11 input variables L[fb -1 ] t-channel cross section [pb] V tb ATLAS ± 2. 4 stat. ± 18. 0(syst.) CMS 5.0 Δσ/σ=19% 9%: I/FSR 9%: b-tag 8%: JES 7%: Gen ± 5. 7 stat. ± syst. ± 4. 0(lumi.) Δσ/σ=16% 8%: JES 6%: Gen. 5%: Muon 5%: b-tag 5%: PDF ± exp. ± 0. 02(th.) Top Quark Production at the LHC 15

16 ATLAS-CONF , CMS PAS TOP R t : ratio of top and anti-top in t-channel R t is sensitive to PDF x [0.02,0.5] can be probed W-charge asymmetry [10-3,10-1 ] at LHC [0.005,0.3] at Tevatron ATLAS@7 TeV: 1.81±0.10 stat. ATLAS: 7 TeV 4.7 fb -1 Fit to NN outputs for l + and l - CMS: 8 TeV 12 fb -1 Fit to h of recoil jets for l + and l - Both results agree with SM predictions CMS@8 TeV: 0.20 (syst.) 1.76±0.14 stat ± (syst) Top Quark Production at the LHC 16

17 Summary Many top measurements from 7 TeV 5 fb -1 of data, and with further statistics of 8 TeV data First LHC σ tt combination Improved σ tt and σ t measurements Large statistics of the LHC sample allows to perform more detailed top measurements Differential cross section Jet multiplicity bb associated with tt R t measurement in t-channel single top Need to improve modeling of the top production in order to be able to probe kinematics regions where new physics may exist More detailed and interesting top results yet to come Top Quark Production at the LHC 17

18 BACKUP SLIDES Top Quark Production at the LHC 18

19 CMS PAS TOP CMS: Vector boson associated with tt 7TeV, 5fb -1 Trilepton approach : tt +Z lvbjjb+ll Same-sign dilepton approach : tt +Z and tt +W σ tt V = stat (syst) pb 4.7σ significance! Top Quark Production at the LHC 19

20 Top Quark Production at the LHC 20

21 Eur. Phys. J. C72 (2012) TeV: Further improvement CMS: σ tt in dilepton with 2.3 fb -1 More refined event selections and analysis techniques, better understanding of systematics Signal extraction by a profile likelihood ratio method to N jets N b jets ± 2. 5 stat (syst) ± 3. 6(lumi) pb Δσ/σ=4.2% Main systematics 2.2% Lumi. 1.9% JES 1.7% BR(W ln) * MADGRAPH used for tt MC Top Quark Production at the LHC 21

22 arxiv: tt with TeV Final state with taus sensitive to charged Higgs CMS: τ+jets in 3.9 fb -1 of data Hadronic τ candidate BDT to separate τ from e/m 4jets ( 1 b-tagged) Largest background from multijet Control sample from untagged data Signal extraction by fitting to Neural Network discriminant 152 ± 12 stat ± 32 syst ± 3 lumi pb Δσ/σ=23% 11% from JES 9% from τ ID Top Quark Production at the LHC 22

23 ATLAS-CONF TeV: tt with semileptonic b-tag ATLAS: 4.7 fb TeV High p T and central lepton(=1) and jets( 3) Soft Muon Tagger (SMT) Uncertainty on σ tt measurement: 1.4% 1.3% from muon identification 0.6% from c 2 matching efficiency Uncorrelated with other b-taggers Cut & count analysis: σ tt = 165 ± 2(stat) ± 17(syst) ± 3(lumi) pb Total uncertainty : 10.5% 6.6% from signal modeling 3.1% from BR(b μx) 5.5% from W+jets estimate 4.4% from multijets estimate SMT b-tagged Signal region Top Quark Production at the LHC 23

24 ATLAS-CONF , CMS PAS TOP TeV: tt in l+jets channel One high p T central lepton, and jets with at least one b-tagged jet Signal extracted by a fit to ATLAS: Likelihood discriminant CMS: M lb distribution 3 jets 4 jets NN-based b-tagger Jet prob. b-tagger Δσ/σ=13% Δσ/σ=13% 11%: signal modeling 8%: b-tag 6%: Jet/E miss T reco. 5%: Jet/E miss T reco. 3.7%: luminosity 4.4%: luminosity L [fb -1 ] σ tt ATLAS ± 2 stat ± 31 syst ± 9(lumi) CMS ± 9 stat syst ± 10(lumi) Top Quark Production at the LHC 24

25 CMS PAS TOP CMS result in dilepton TeV 2.4 fb -1 of data A simple and robust cut&count Analysis baseline is the same as 7 TeV analysis Channel ee mm em ll Cross section [pb] 231 ± 8 stat ± 15 syst ± 10(lumi) 220±6 stat ± 15 syst ± 10(lumi) 227 ± 4(stat) ± 11(syst) ± 10(lumi) 227 ± 3(stat) ± 11(syst) ± 10(lumi) Δσ/σ =6.7% 4.4% from luminosity 2.5% from JES Top Quark Production at the LHC 25

26 Jet multiplicity in 7 TeV, 5 fb -1, dilepton channels Unfolded jet multiplicities comparing with several QCD calculations MadGraph and POWHEG describe well the data MC@NLO generates lower multiplicities than observed Top Quark Production at the LHC 26

27 8 TeV: tt with b-tagging at ATLAS Use 5.8 fb -1 of data High p T and central lepton(=1) and jets( 3) At least one b-tagged jet Use neural network-based tagger Signal extraction by fitting to a likelihood discriminant (lepton rapidity, aplanarity) Δσ/σ=13% 1. 11% from signal modeling 2. 6% from Jet/E T miss reco % from luminosity ATLAS-CONF σ tt = 241 ± 2(stat. ) ± 31(syst.) ± 9(lumi.) pb Top Quark Production at the LHC 27

28 8 TeV: tt with b-tagging at CMS Up to 2.8 fb -1 of data High p T and central lepton(=1) and jets( 4) At least one b-tagged jet Signal extraction by fitting to M lb distribution Δσ/σ=13% 8% from b-tag 5% from Jet/E T miss reco. 4.4% from luminosity CMS PAS TOP σ tt = ± 9. 0 stat syst. ± lumi. pb Top Quark Production at the LHC 28

29 ATLAS-CONF R t : ratio of top and anti-top in t-channel R t is sensitive to PDF x [0.02,0.5] can be probed W-charge asymmetry [10-3,10-1 ] at LHC [0.005,0.3] at Tevatron ATLAS: 4.7 fb -1 of 7TeV data Signal extraction by fitting NN outputs top quark anti-top quark σ(t) σ(t ) 53.2±1.7 stat. ±10.6 syst. pb 29.5±1.5 stat. ±7.3 syst. pb R t 1.81±0.10 stat (syst.) Δσ(t)/σ(t)=20%, Δσ(t )/σ(t)=25% (JES is dominant: 16 20%) ΔR t /R t =13% (6% Stat., 4% for MC stat., Bkg, JES, ISR/FSR ) Top Quark Production at the LHC 29

30 CMS PAS TOP R t measurement at 8 TeV CMS: 8 TeV, 12 fb -1 Signal extraction by a fit to η distributions of recoil jet for l + and l -, simultaneously σ(t) σ(t ) R t 49.6±2. 0 stat ±8. 8 syst pb 28.2±2. 2 stat ±4. 8 syst pb 1.76±0.14 stat ± (syst) Δσ(t)/σ(t)=18%, Δσ(t )/σ(t )=19% Signal modeling is dominant: 11 15% ΔR t /R t =15% 9% from data stat. 8% from PDF 7% from W+jets, tt extraction top quark anti-top quark Top Quark Production at the LHC 30

31 Top Quark Production at the LHC 31

32 Top Quark Production at the LHC 32

33 Top Quark Production at the LHC 33

34 Top Quark Production at the LHC 34

35 Top Quark Production at the LHC 35

36 Top Quark Production at the LHC 36

37 Top Quark Production at the LHC 37

38 Top Quark Production at the LHC 38

39 Top event in the detector 33% 67% tt analysis modes e/m + jets 34.3% All hadronic 59.2% ee/mm/em 6.4% *t is considered as either hadronic or e/m Top Quark Production at the LHC 39

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

The 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 information

W/Z + jets and W/Z + heavy flavor production at the LHC

W/Z + jets and W/Z + heavy flavor production at the LHC W/Z + jets and W/Z + heavy flavor production at the LHC A. Paramonov (ANL) on behalf of the ATLAS and CMS collaborations Moriond QCD 2012 Motivation for studies of jets produced with a W or Z boson Standard

More information

Highlights of top quark measurements in hadronic final states at ATLAS

Highlights 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 information

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

The Compact Muon Solenoid Experiment. Conference Report. Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland Available on CMS information server CMS CR -2017/094 The Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH211 GENEVA 23, Switzerland 18 March 2017 (v3, 20 March 2017) Recent

More information

Top production measurements using the ATLAS detector at the LHC

Top 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 information

PoS(CKM2016)117. Recent inclusive tt cross section measurements. Aruna Kumar Nayak

PoS(CKM2016)117. Recent inclusive tt cross section measurements. Aruna Kumar Nayak Recent inclusive tt cross section measurements Institute of Physics, Bhubaneswar, India E-mail: Aruna.Nayak@cern.ch Results of the recent measurements for the inclusive tt production cross section in the

More information

Inclusive 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 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 information

Highlights of top-quark measurements in hadronic nal states at ATLAS

Highlights 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 information

Recent Results on Top Physics at CMS

Recent 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 information

tt + X production at ATLAS and CMS

tt + X production at ATLAS and CMS tt + X production at ATLAS and CMS Antonio Sidoti on behalf of the ATLAS and CMS collaborations Istituto Nazionale Fisica Nucleare Sezione di Bologna Top quark Try to avoid repetitions with M. Aldaya Martin

More information

Physics with Tau Lepton Final States in ATLAS. Felix Friedrich on behalf of the ATLAS Collaboration

Physics 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 information

Top quark pair cross section measurements at the Tevatron experiments and ATLAS. Flera Rizatdinova (Oklahoma State University)

Top quark pair cross section measurements at the Tevatron experiments and ATLAS. Flera Rizatdinova (Oklahoma State University) Top quark pair cross section measurements at the Tevatron experiments and ATLAS (Oklahoma State University) Outline Introduction: Large Hadron Collider (LHC) and major experiments on it ATLAS detector

More information

arxiv: v1 [hep-ex] 8 Jan 2018

arxiv: v1 [hep-ex] 8 Jan 2018 Top mass measurements in ATLAS and CMS arxiv:8.239v [hep-ex] 8 Jan 28 A. CASTRO University of Bologna and INFN, Bologna, Italy On behalf of the ATLAS and CMS Collaborations Abstract Top quarks are produced

More information

Measurement of t-channel single top quark production in pp collisions

Measurement of t-channel single top quark production in pp collisions Measurement of t-channel single top quark production in pp collisions (on behalf of the CMS collaboration) INFN-Napoli & Università della Basilicata E-mail: Francesco.Fabozzi@cern.ch Measurements of t-channel

More information

Physics at Hadron Colliders

Physics 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 information

Top properties and ttv LHC

Top properties and ttv LHC Top properties and ttv results @ LHC Emmanuel MONNIER CPPM/IN2P3 Aix-Marseille Université (Marseille, FRANCE) On behalf of the ATLAS and CMS collaborations 15 March 2016 Moriond EW@La Thuile a Many top

More information

Combination of top quark physics results at the LHC

Combination of top quark physics results at the LHC Combination of top quark physics results at the LHC María Aldaya (DESY) for the CMS & ATLAS Collaborations within the TOPLHCWG ICHEP 2014, Valencia, 2-9 July 2014 What is the TOPLHCWG? http://lpcc.web.cern.ch/lpcc/

More information

Single top: prospects at LHC

Single top: prospects at LHC Single top: prospects at LHC Markus Cristinziani (Uni Bonn) for ATLAS, Giovanni Petrucciani (SNS & INFN Pisa) for CMS Top2008 M. Cristinziani (Bonn), G. Petrucciani (Pisa) 1 Outline What changes between

More information

Top production at the Tevatron

Top 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 information

Search for the Higgs boson in the t th production mode using the ATLAS detector

Search for the Higgs boson in the t th production mode using the ATLAS detector Search for the Higgs boson in the t th production mode using the ATLAS detector Rustem Ospanov (University of Pennsylvania) on behalf of the ATLAS collaboration Large Hadron Collider Physics Conference,

More information

arxiv: v1 [hep-ex] 28 Aug 2017

arxiv: v1 [hep-ex] 28 Aug 2017 Proceedings of the Fifth Annual LHCP AL-PHYS-PROC-7-99 November 9, 8 Boosted top production in ALAS and arxiv:78.864v [hep-ex] 8 Aug 7 Marino Romano On behalf of the ALAS and Collaborations, INFN, Sezione

More information

Measurements of the production of a vector boson in association with jets in the ATLAS and CMS detectors

Measurements of the production of a vector boson in association with jets in the ATLAS and CMS detectors Measurements of the production of a vector boson in association with s in the ALAS and CMS detectors Vieri Candelise University of rieste and INFN rieste, Via Valerio 2, 3428, rieste, Italy Abstract. he

More information

Top results from CMS

Top results from CMS Top results from CMS Alicia Calderon Instituto de Fisica de Cantabria (CSIC - University of Cantabria) Avda. Los Castros, s.n. Santander, SPAIN On behalf of the CMS collaboration. 1 Introduction The top

More information

Top Quark Physics at LHC

Top Quark Physics at LHC Top Quark Physics at LHC Frank-Peter Schilling Karlsruhe Institute of Technology (KIT) (on behalf of the ATLAS, CMS collaborations) QCD@LHC, East Lansing (US) August 2012 Outline ttbar total cross section

More information

Top quark mass at ATLAS and CMS

Top 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 information

ATLAS Measurements of Boosted Objects

ATLAS Measurements of Boosted Objects BOOS24 University College London, 8-22 August 24 ALAS Measurements of Boosted Objects Christoph Anders on behalf of the ALAS collaboration Physikalisches Institut Universita t Heidelberg August 9th 24

More information

PDF Studies at LHCb! Simone Bifani. On behalf of the LHCb collaboration. University of Birmingham (UK)

PDF 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 information

Measurement 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 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 information

NEW RESULTS FROM THE TOP QUARK

NEW RESULTS FROM THE TOP QUARK NEW RESULTS FROM THE TOP QUARK Thomas Muller, Institut für Experimentelle Kernphysik, KIT Fermilab Tevatron CERN Large Hadron Collider Tevatron: Run 1: s = 1.8 TeV (1992-1996) Top quark discovery in 1995

More information

Physics at Tevatron. Koji Sato KEK Theory Meeting 2005 Particle Physics Phenomenology March 3, Contents

Physics 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 information

PANIC August 28, Katharina Müller on behalf of the LHCb collaboration

PANIC August 28, Katharina Müller on behalf of the LHCb collaboration Measurements with electroweak bosons at LHCb PANIC August 28, 2014 on behalf of the LHCb collaboration Outline LHCb detector Measurements with electroweak bosons Motivation Z production Z plus jets, Z

More information

Single top quark production at CDF

Single top quark production at CDF Available online at www.sciencedirect.com Nuclear and Particle Physics Proceedings 73 75 (16) 74 79 www.elsevier.com/locate/nppp Single top quark production at CDF Sandra Leone, on behalf of the CDF Collaboration

More information

Top Quark Studies with CMS

Top Quark Studies with CMS Top Quark Studies with CMS Frank-Peter Schilling (KIT) on behalf of the CMS collaboration The TOP Top Physics at the LHC Precise SM measurements o Heaviest known elementary particle (large Yukawa coupling)

More information

Electroweak results. Luca Lista. INFN - Napoli. LHC Physics

Electroweak 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 information

ATLAS-CONF October 15, 2010

ATLAS-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 information

Differential Top Cross-section Measurements

Differential Top Cross-section Measurements Differential op Cross-section Measurements ALPS207 Obergurgl Michael Fenton on behalf of the ALAS Collaboration University of Glasgow m.fenton.@research.gla.ac.uk April 8, 207 Michael Fenton Differential

More information

Top and Electroweak Physics at. the Tevatron

Top 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 information

CDF top quark " $ )(! # % & '

CDF 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 information

tt production in the forward region at LHCb

tt production in the forward region at LHCb tt production in the forward region at LHCb María Vieites Díaz, On behalf of the LHCb Collaboration Universidade de Santiago de Compostela image from https://www.trada.co.uk/case-studies/the-globe-at-cern-geneva/

More information

PoS(HQL 2016)039. Top quark properties. Javier Cuevas Maestro U de Oviedo

PoS(HQL 2016)039. Top quark properties. Javier Cuevas Maestro U de Oviedo U de Oviedo E-mail: fjcuevas@uniovi.es An overview of recent top quark measurements in proton-proton collisions at s = 7, 8 TeV in data collected with the CMS and ATLAS experiments at the LHC, using a

More information

Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy

Proton 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 information

Review of LHCb results on MPI, soft QCD and diffraction

Review of LHCb results on MPI, soft QCD and diffraction Review of LHCb results on MPI, soft QCD and diffraction Marcin Kucharczyk on behalf of LHCb collaboration HNI Krakow EDS Blois 2015, Borgo (Corse), 30.06.2015 Outline LHCb - general purpose forward experiment

More information

Recent ATLAS measurements in Higgs to diboson channels

Recent ATLAS measurements in Higgs to diboson channels Recent ATLAS measurements in Higgs to diboson channels Yusheng Wu University of Michigan Institute of Physics, Academia Sinica On behalf of the ATLAS collaboration August 31 st - Higgs Hunting 2016 Introduction

More information

Measurement of EW production! of Z+2j at the LHC

Measurement of EW production! of Z+2j at the LHC Measurement of EW production! of Z+j at the LHC Frontiers of Fundamental Physics, Marseille Kiran Joshi On behalf the ATLAS and CMS collaborations /7/ Overview Introduction and motivation ATLAS measurement

More information

Single Top t -Channel

Single Top t -Channel On behalf of the ATLAS and CMS collaborations LHCP 15, St. Petersburg Single Top t -Channel Benedikt Maier Institute for Experimental Nuclear Physics 1 Things to Measure in tchannel inclusive and differential

More information

Top quark at LHC. M. Villa. Bologna, oggi

Top quark at LHC. M. Villa. Bologna, oggi Top quark at LHC M. Villa Bologna, oggi 1 Outline Top quark characteristics Top production and decay Measurements 2 Outline Top quark characteristics Top production and decay Measurements 3 Top quark I.D.

More information

W/Z+jet results from the Tevatron

W/Z+jet results from the Tevatron W/Z+jet results from the Tevatron Dmitry Bandurin Florida State University On behalf of D0 and CDF Collaborations Moriond QCD 2012, March 15, La Thuile, Italy Precision QCD tests Photon, W, Z etc. p parton

More information

Electroweak Measurements at LHCb!

Electroweak 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 information

Measurements of the tt Cross Section and Top Mass at CDF

Measurements 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 information

Determination of the Top- Quark Mass from the m lb Distribution in Dileptonic Top-Pair Events at s= 8 TeV

Determination of the Top- Quark Mass from the m lb Distribution in Dileptonic Top-Pair Events at s= 8 TeV Deteration of the Top- Quark Mass frohe Distribution in Dileptonic Top-Pair Events at s= 8 TeV.1.14 - Motivation - - Event Selection & mlb Definition- - Extraction: Method - - Results - - Summary - 1 Motivation

More information

La ricerca dell Higgs Standard Model a CDF

La 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 information

Measurement of the jet production properties at the LHC with the ATLAS Detector

Measurement of the jet production properties at the LHC with the ATLAS Detector Measurement of the jet production properties at the LHC with the ALAS Detector Stanislav okar Comenius University, Bratislava On behalf of the ALAS collaboration Different features of the jet production

More information

Results on top physics by CMS

Results on top physics by CMS EPJ Web of Conferences 95, 04069 (2015) DOI: 10.1051/ epjconf/ 20159504069 C Owned by the authors, published by EDP Sciences, 2015 Results on top physics by CMS Silvano Tosi 1,2,a, on behalf of the CMS

More information

Searches for exotica at LHCb

Searches for exotica at LHCb Searches for exotica at LHCb Lorenzo Sestini Università di Padova e INFN LHCb Implications Workshop, Geneve-Cern, 3-11-2015 Searches for exotics LHCb can be complementary to ATLAS and CMS in the search

More information

Inclusive. W & Z measurements in CMS. Georgios Daskalakis. on behalf of CMS Collaboration. .C.S.R. Demokritos

Inclusive. 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 information

Measurements of the vector boson production with the ATLAS detector

Measurements of the vector boson production with the ATLAS detector Measurements of the vector boson production with the ATLAS detector A. Lapertosa 1,2,, on behalf of the ATLAS Collaboration 1 Università degli Studi di Genova 2 INFN Sezione di Genova Abstract. Measurements

More information

QCD Multijet Background and Systematic Uncertainties in Top Physics

QCD Multijet Background and Systematic Uncertainties in Top Physics QCD Multijet Background and Systematic Uncertainties in Top Physics Jin Wang On behalf of ATLAS, CMS, CDF and D0 Collaborations IHEP, China 2013-09-15, Top2013 1 Outline Introduction of QCD Multijet Background

More information

Study of Higgs boson leptonic decay modes

Study of Higgs boson leptonic decay modes Study of Higgs boson leptonic decay modes Windows on the Universe ICSE, Vietnam 11-17.08.2013 Pawel Brückman de Renstrom on behalf of the ATLAS, CMS, CDF, D0 Collaborations ( Institute of Nuclear Physics

More information

Evidence for tth production at ATLAS

Evidence for tth production at ATLAS Evidence for tth production at ATLAS Rohin T Narayan on behalf of the ATLAS collaboration Nov-6-2017, Higgs couplings Heidelberg Motivation Fermion masses are generated through Yukawa interaction Heaviest

More information

Top Quark Physics at the LHC

Top Quark Physics at the LHC Top Quark Physics at the LHC Ayana Arce HEP 0 Lectures #7 March 4, 203 Outline Introduction 2 Why are top quarks interesting? 3 Creating Top Quarks 4 Identifying Top Quarks 5 Some LHC results 6 Beyond

More information

NEWS FROM THE TOP. 1. Pair Production of Top Quarks Cross Section Search for Resonances Forward-Backward Asymmetry

NEWS 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 information

W, Z and top production measurements at LHCb

W, 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 information

Precision 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 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 information

Single top production at ATLAS and CMS. D. Lontkovskyi on behalf of the ATLAS and CMS Collaborations La Thuile, March, 2018

Single top production at ATLAS and CMS. D. Lontkovskyi on behalf of the ATLAS and CMS Collaborations La Thuile, March, 2018 Single top production at ATLAS and CMS D. Lontkovskyi on behalf of the ATLAS and CMS Collaborations La Thuile, 17-24 March, 2018 1 Single top quark production at the LHC LHC is the top factory Large integrated

More information

Moriond QCD. Latest Jets Results from the LHC. Klaus Rabbertz, KIT. Proton Structure (PDF) Proton Structure (PDF) Klaus Rabbertz

Moriond QCD. Latest Jets Results from the LHC. Klaus Rabbertz, KIT. Proton Structure (PDF) Proton Structure (PDF) Klaus Rabbertz Latest Jets Results from the LHC Proton Structure (PDF) Proton Structure (PDF), KIT 1 Flash Menu Motivation Accelerators and Detectors Jet Algorithms and Calibration Inclusive Jets Dijets and 3-Jets The

More information

B-Tagging in ATLAS: expected performance and and its calibration in data

B-Tagging in ATLAS: expected performance and and its calibration in data B-Tagging in ATLAS: expected performance and and its calibration in data () on behalf of the ATLAS Collaboration Charged Higgs 2008 Conference (Uppsala: 15-19 September 2008) Charged Higgs Conference -

More information

arxiv: v1 [hep-ex] 27 Nov 2017

arxiv: v1 [hep-ex] 27 Nov 2017 CDF note 11237 November 28, 2017 Top quark properties at Tevatron arxiv:1711.09686v1 [hep-ex] 27 Nov 2017 Roman Lysák on behalf of the CDF and D0 collaborations Institute of Physics of the Czech Academy

More information

PoS(EPS-HEP 2013)215. WW, WZ, and ZZ production at CMS. Jordi DUARTE CAMPDERROS (on behalf of CMS collaboration)

PoS(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 information

High p T physics at the LHC Lecture III Standard Model Physics

High p T physics at the LHC Lecture III Standard Model Physics High p T physics at the LHC Lecture III Standard Model Physics Miriam Watson, Juraj Bracinik (University of Birmingham) Warwick Week, April 2011 1. LHC machine 2. High PT experiments Atlas and CMS 3. Standard

More information

Recent QCD results from ATLAS

Recent QCD results from ATLAS Recent QCD results from ATLAS PASCOS 2013 Vojtech Pleskot Charles University in Prague 21.11.2013 Introduction / Outline Soft QCD: Underlying event in jet events @7TeV (2010 data) Hard double parton interactions

More information

First 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, 8-10 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 information

Search for tt(h bb) using the ATLAS detector at 8 TeV

Search for tt(h bb) using the ATLAS detector at 8 TeV Search for tt(h bb) using the ATLAS detector at 8 TeV on behalf of the ATLAS Collaboration University of Göttingen Motivation, Strategy & Introduction Overview: tt(h bb) leptonic analysis Summary & Outlook

More information

Yoshikazu NAGAI (CPPM, Aix Marseille Université)

Yoshikazu NAGAI (CPPM, Aix Marseille Université) Search for the Standard Model Higgs boson decaying into a b quark pair at ATLAS Yoshikazu NAGAI (CPPM, Aix Marseille Université) CPPM Seminar October 20, 2014 Contents Introduction Analysis overview Result

More information

QCD and Top physics studies in proton-proton collisions at 7 TeV centre-of-mass energy with the ATLAS detector

QCD and Top physics studies in proton-proton collisions at 7 TeV centre-of-mass energy with the ATLAS detector Journal of Physics: Conference Series QCD and Top physics studies in proton-proton collisions at 7 TeV centre-of-mass energy with the ATLAS detector To cite this article: Marcello Barisonzi 2012 J. Phys.:

More information

Latest results on the SM Higgs boson in the WW decay channel using the ATLAS detector

Latest results on the SM Higgs boson in the WW decay channel using the ATLAS detector Latest results on the SM iggs boson in the decay channel using the detector arxiv:188.954, accepted by PRB Claudia Bertella, on behalf of Collaboration The 4th China LC Physics Workshop (CLCP 218) 21-December-218

More information

arxiv: v1 [hep-ex] 16 Jan 2019

arxiv: v1 [hep-ex] 16 Jan 2019 CMS-CR-28/262 January 7, 29 Measurement of the single top quark and antiquark production cross sections in the t channel and their ratio at TeV arxiv:9.5247v [hep-ex] 6 Jan 29 Denise Müller on behalf of

More information

Double Parton Scattering in CMS. Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x th June 2017 Bari, Italy

Double Parton Scattering in CMS. Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x th June 2017 Bari, Italy Double Parton Scattering in CMS Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x 2017 17th June 2017 Bari, Italy Outline Introduction to DPS DPS measurements with CMS 2b +

More information

Measurement of the jet mass distribution in boosted top quark decays at 8 TeV in CMS

Measurement of the jet mass distribution in boosted top quark decays at 8 TeV in CMS Measurement of the jet mass distribution in boosted top quark decays at 8 TeV in CMS, Johannes Haller, Roman Kogler itroduction jet mass mjet: invariant mass of all stable particles in a jet boosted top

More information

B-quark discovery. e+ e- PETRA GeV TRISTAN 61.4 GeV LEP Mz Mt > 45.8 GeV

B-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 information

Frédéric Derue Laboratoire de Physique Nucléaire et de Hautes Energies ( LPNHE) Paris on behalf of the ATLAS Collaboration

Frédéric Derue Laboratoire de Physique Nucléaire et de Hautes Energies ( LPNHE) Paris on behalf of the ATLAS Collaboration Latest ATLAS measurements on top quark properties (excluding single top) Frédéric Derue Laboratoire de Physique Nucléaire et de Hautes Energies ( LPNHE) Paris on behalf of the ATLAS Collaboration 10th

More information

Direct measurement of the W boson production charge asymmetry at CDF

Direct 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 information

Outline. Heavy elementary particles. HERA Beauty quark production at HERA LHC. Top quark production at LHC Summary & conclusions

Outline. Heavy elementary particles. HERA Beauty quark production at HERA LHC. Top quark production at LHC Summary & conclusions Outline Heavy elementary particles HERA Beauty quark production at HERA LHC Charm, beauty (bottom) and truth (top) Status and plans Top quark production at LHC Summary & conclusions 2 Elementary Particles

More information

Discussion of QCD aspects of multi boson production measured with the ATLAS detector

Discussion of QCD aspects of multi boson production measured with the ATLAS detector Discussion of QCD aspects of multi boson production measured with the ATLAS detector Dimos Sampsonidis Aristotle University of Thessaloniki On behalf of the ATLAS Collaboration Low-x Meeting 2016, 6-11

More information

arxiv: v1 [hep-ex] 12 Sep 2014

arxiv: v1 [hep-ex] 12 Sep 2014 op Quark Measurements in CMS Efe Yazgan a, a Department of Physics and Astronomy, Ghent University, Proeftuinstraat 86 B-9 Gent, Belgium. arxiv:9.3737v [hep-ex] Sep Abstract Measurements involving top

More information

PoS(ICHEP2012)311. Identification of b-quark jets in the CMS experiment. Sudhir Malik 1

PoS(ICHEP2012)311. Identification of b-quark jets in the CMS experiment. Sudhir Malik 1 Identification of b-quark jets in the CMS experiment 1 University of Nebraska-Lincoln Lincoln, NE 68588 E-mail: malik@fnal.gov The identification of jets arising from the production of b-quarks is an essential

More information

tth searches at ATLAS and CMS Thomas CALVET for the ATLAS and CMS collaborations Stony Brook University Apr 11 th, 2018

tth searches at ATLAS and CMS Thomas CALVET for the ATLAS and CMS collaborations Stony Brook University Apr 11 th, 2018 tth searches at ATLAS and CMS Thomas CALVET for the ATLAS and CMS collaborations Stony Brook University SM@LHC2018 Apr 11 th, 2018 Cross-section (pb) The Higgs Top Sector Higgs boson discovery in 2012

More information

Pursuing EWK Symmetry Breaking at CDF

Pursuing EWK Symmetry Breaking at CDF Pursuing EWK Symmetry Breaking at CDF Standard Model EWK Symmetry Breaking Status of Tevatron running Top Quark properties Top Mass measurement Standard Model Higgs Searches Summary 1 Standard Model The

More information

SOFT QCD AT ATLAS AND CMS

SOFT QCD AT ATLAS AND CMS SAHAL YACOOB UNIVERSITY OF CAPE TOWN ON BEHALF OF THE ATLAS AND CMS COLLABORATIONS SOFT QCD AT ATLAS AND CMS 28th Rencontres de Blois INTRODUCTION IN 15 MINUTES 2 Inelastic cross section ATLAS and CMS

More information

Higgs searches in TauTau final LHC. Simone Gennai (CERN/INFN Milano-Bicocca) Mini-workshop Higgs Search at LHC Frascati, March 28th, 2012

Higgs searches in TauTau final LHC. Simone Gennai (CERN/INFN Milano-Bicocca) Mini-workshop Higgs Search at LHC Frascati, March 28th, 2012 Higgs searches in TauTau final states @ LHC Simone Gennai (CERN/INFN Milano-Bicocca) Mini-workshop Higgs Search at LHC Frascati, March 28th, 2012 1 Motivations Why looking at H->TauTau? second highest

More information

Bill Murray Warwick University / RAL, STFC On behalf of the ATLAS and CMS collaborations 26th March 2017

Bill Murray Warwick University / RAL, STFC On behalf of the ATLAS and CMS collaborations 26th March 2017 s w g i t g h i H W. Murray 1 S i g c n i a n t o u r r d es a H Bill Murray Warwick University / RAL, STFC On behalf of the ATLAS and CMS collaborations 26th March 2017 H bb in th,vbf, VH and tth W. Murray

More information

W. Fedorko for the ATLAS collaboration

W. Fedorko for the ATLAS collaboration W. Fedorko for the ATLAS collaboration The Standard Model very well tested BUT: No way to incorporate gravity No viable dark matter candidate Hierarchy problem W. Fedorko High Mass resonances at ATLAS

More information

Search for Fermionic Higgs Boson Decays in pp Collisions at ATLAS and CMS

Search for Fermionic Higgs Boson Decays in pp Collisions at ATLAS and CMS Higgs boson searches in fermionic final state at LHC Search for Fermionic Higgs Boson Decays in pp Collisions at ATLAS and CMS Romain Madar on behalf of ATLAS and CMS collaboration Physikalisches Institut

More information

PoS(ICHEP2012)300. Electroweak boson production at LHCb

PoS(ICHEP2012)300. Electroweak boson production at LHCb Physik-Institut der Universität Zürich, Switzerland. E-mail: jonathan.anderson@cern.ch The electroweak boson production cross-sections have been measured in the forward region using s = 7 TeV proton-proton

More information

Recent Results from CDF. Gabriele Compostella (INFN and University of Padova) on behalf of the CDF Collaboration

Recent Results from CDF. Gabriele Compostella (INFN and University of Padova) on behalf of the CDF Collaboration Recent Results from CDF Gabriele Compostella (INFN and University of Padova) on behalf of the CDF Collaboration XCVI Congresso Nazionale della Società Italiana di Fisica - Bologna, 20-24 Settembre, 2010

More information

VBF SM Higgs boson searches with ATLAS

VBF SM Higgs boson searches with ATLAS VBF SM Higgs boson searches with Stefania Xella (for the collaboration) Niels Bohr Institute, Copenhagen University, Denmark E-mail: xella@nbi.dk The observation of a Standard Model Higgs boson produced

More information

Measurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV

Measurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV Measurement of Jet Energy Scale and Resolution at ATLAS and CMS at s = 8 TeV EDSBlois 2015 02.07.2015 Dominik Haitz on behalf of the ATLAS and CMS Collaborations INSTITUT FÜR EXPERIMENTELLE KERNPHYSIK

More information

QCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations

QCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations QCD Jets at the LHC Leonard Apanasevich University of Illinois at Chicago on behalf of the ATLAS and CMS collaborations Outline Physics at the LHC Jet Reconstruction and Performance Clustering Algorithms

More information

Tests of QCD Using Jets at CMS. Salim CERCI Adiyaman University On behalf of the CMS Collaboration IPM /10/2017

Tests of QCD Using Jets at CMS. Salim CERCI Adiyaman University On behalf of the CMS Collaboration IPM /10/2017 Tests of QCD Using Jets at CMS Salim CERCI Adiyaman University On behalf of the CMS Collaboration IPM-2017 24/10/2017 2/25 Outline Introduction QCD at LHC QCD measurements on the LHC data Jets The strong

More information

Top Physics in Hadron Collisions

Top 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 information

Search for Higgs to tt at CMS

Search for Higgs to tt at CMS Search for Higgs to tt at CMS Arun Nayak IRFU/SPP, CEA, Saclay 11/10/2013 Aperos du SPP 1 Why Higgs to tt? Introduction Most sensitive channel to probe lepton couplings o Important to establish SM predictions

More information