Search for Higgs Bosons produced in associa3on with top quarks with the ATLAS detector

Size: px
Start display at page:

Download "Search for Higgs Bosons produced in associa3on with top quarks with the ATLAS detector"

Transcription

1 Search for Higgs Bosons produced in associa3on with top quarks with the ATLAS detector Marine Kuna (INFN Roma) On behalf of The ATLAS Collabora3on Phenomenology 2015, PiOsburgh May 4, 2015 Marine Kuna - OH ATLAS - PHENO

2 Mo3va3ons Ø Discovery of a Higgs boson compa3ble with the Standard Model à proper3es measurement Coupling to other par3cles Propor3onal to the fermion s mass à strongest is coupling to top quark Ø Higgs produced in associa3on with a top quark pair (OH) allows direct access to Yukawa coupling of Higgs boson to top quark 4H (0.6%) Gluon fusion pp) top? v V m κ V or v F m κ F 1 10 ATLAS Preliminary s = 7 TeV, fb s = 8 TeV, 20.3 fb Observed SM Expected W Z t Ø OH analyses also sensi3ve to th: If κ f =- 1, κ v =1 (construc3ve interference) à ~13*σ th κ v µ τ b λ f = 2 m f ν Particle mass [GeV] 2 κ f Ø coupling strengths κ X 2 = Γ H X SM Γ H X à Any devia3on might be hint for new physics 2 Marine Kuna - OH ATLAS - PHENO 2015

3 Analysis Overview tth γγ Best mass peak resolu3on High signal purity But low branching frac3on: BR(Hà γγ)~0.2% Physics Le*ers B 740 (2015) L = 25 _ - 1 (7 & 8 TeV) g g _ t t H W _ b b W tth bb Highest branching frac3on But important Obar +heavy/light flavour background ATLAS- HIGG submi*ed to EPJC L = 20 _ - 1 (8 TeV) tth multileptons (WW/ττ/ZZ) Best theore3cal handle on background ATLAS- CONF L = 20 _ - 1 (8 TeV) Combina3on ATLAS- CONF L = 25 _ - 1 (7 & 8 TeV) Good signal purity and branching ra3o compromise But too low sta3s3cs Marine Kuna - OH ATLAS - PHENO

4 OHà γγ TeV tth γγ Ø Inclusive Hà γγ analysis (sideband fit for background) + addi3onal requirements for 2 categories depending on top pair decay: hadronic leptonic (semi or fully) H no lepton 6 jets 2 b- tag 1 lepton 1 b- tag E T miss > 20 GeV Ø Results on signal strength µ = µ OH =σ(oh)/σ(oh) SM Limit: µ OH (σ/σ SM ) < 6.7 obs (4.9 CL Measured µ: µ = (stat.) +0.8 (syst.) Ø Taking into account OH and th cross sec3ons dependence, also sets limits on coupling strength: κ t [ 1.3; CL Marine Kuna - OH ATLAS - PHENO

5 OHà bb 8 TeV tth bb Ø 2 Sub- Channels according to top pair decay modes: single lepton & dilepton Ø Both rely on (N jets, N b- tags ) categorisa3on to get signal enriched regions to enhance sensi3vity, and background- rich regions to beoer constrain backgrounds normalisa3on Ø Discriminants are: à For low signal rate regions: H T /H had t (di- lep/single- lep) Single- lep 4j 4b illustraeon à For high sensi3vity regions: Neural Network (NN) Dilep 3j 3b illustraeon Discriminants in each category: illustraeon for single- lep channel ATLAS Simulation Single lepton s = 8 TeV, 20.3 fb = 125 GeV m H N b- tag 4 S / B j, 2 b S/B < 0.1% B S / j, 3 b S/B = 0.2% B S / H had T H had T H had T j, 4 b S/B = 1.4% H T had : Σ p T (jets) 5 B S / j, 2 b S/B = 0.1% H T had B S / j, 3 b S/B = 0.4% NNHF B S / j, 4 b S/B = 2.5% NN H T : Σ p T (jets, leptons) 6 B S / N jets Marine Kuna - OH ATLAS - PHENO j, 2 b S/B = 0.2% H T had B S / j, 3 b S/B = 1.0% NN[ME] B S / j, 4 b S/B = 4.0% NN[ME]

6 Neural Network Discriminants 8 TeV tth bb Ø Neural Networks (NN) using kinema3c informa3on trained in each category 7 variables used to separate O+HF (heavy flavour) from O+light in 5j3b single- lep region Other NN regions use 10 or 12 variables to dis3nguish signal from background (mainly O+bb con3nuum) Matrix Element p T of fith leading jet IllustraEon for 6j, 4b single lepton category + 9 other variables 2 Matrix Elements variables added in single lep 6j3b & 6j4b (probability density funceon of integral over phase space of all inieal and final state parecles) Σp T /E for jets and leptons Marine Kuna - OH ATLAS - PHENO

7 Main Systema3cs and Results 8 TeV tth bb Ø Main background O+bb (Powheg+Pythia6 reweighted to Sherpa OpenLoops), 50% theory unc. constrained 15% (30% for O+cc) Ø Leading systema3cs: O+bb/cc normalisa3ons and modelling, Jet Energy Scale, mis- tag from O+light flavours µ = 1.5 ±1.1 µ OH (σ/σ SM ) < 3.4 obs (2.2 CL Dilepton Lepton+jets ATLAS tth (H bb) s=8 TeV, 20.3 fb Expected ± 1σ Expected ± 2σ Dilepton Lepton+jets ( tot ) ( stat ) 2.8 ± 2.0 ( 1.4 ) 1.2 ± 1.3 ( 0.8 ) Observed Combination Combination 1.5 ± 1.1 ( 0.7 ) Injected signal (µ=1) Best fit µ=σ/σ for m H =125 GeV SM 95% CL limit on σ/σ SM at m H =125 GeV Marine Kuna - OH ATLAS - PHENO 2015 tot. stat. ATLAS tth (H bb ) s=8 TeV, 20.3 fb 7

8 OHà mul3leptons 8 TeV tth multilep Ø 5 Channels orthogonal in light leptons and hadronic tau mul3plicity N hadronic taus (τ had ) l+2τ had SS: Same Sign 2lSS+1τ had 2lSS 6 categories: (==4, 5 jets) x (ee, eµ, µµ) 3l 4l 2 categories: Z depleted & Z enriched N light leptons (l) g KH(ττ) à 2l+τ had t 8 TeV Reject Obar background with: same sign di- leptons N lep 3 W + q b q Ø Sensi3vity to WW, ττ and ZZ Higgs decays H τ + τ + had ν τ Ordered by sensi3vity g t τ W l ν l ν τ b l ν l Marine Kuna - OH ATLAS - PHENO

9 2lSS+1τhad event display 8 TeV tth multilep In final state: 1 electron, 1 muon, 1 hadronic tau and 4 jets of which 2 b- tag 8 TeV Marine Kuna - OH ATLAS - PHENO

10 Main Backgrounds and Systema3cs 8 TeV tth multilep Ø Charge mis- iden3fica3on data driven, extrapola3on from Zà ee (only for 2l) Ø Non- Prompt (reducible, mainly Obar) from data, es3mated 8 TeV from extrapola3on from Control Regions with reversed lepton isola3on, ID variables and p T Ø OW, OZ (irreducible) from Monte Carlo (MC) + Data/MC agreement checks in Ø VV (diboson) from MC various Valida3on Regions Impact on signal strength uncertainty * * * *detector and reconstruceon systemaecs Events s = 8 TeV, 20.3 fb ATLAS Preliminary 2l0 Non-Prompt had category Charge misid tth(125) Data Number of jets Marine Kuna - OH ATLAS - PHENO Rare VV ttz ttw

11 Results 8 TeV tth multilep Ø Cut and count analysis: µ OH (σ/σ SM ) < 4.7 obs (2.4 CL Channel SM Higgs Backgrounds Data 2lSS+0τ had 6.6±1.4 77± l 11.4± ± lSS+1τ had 0.47±2 1.4± l 0.20±1 0.55± l+2τ had 0.68±7 16± TeV Slight excess in leptonic- only channels, deficit in hadronic tau channels 1l2τ had s = 8 TeV, L dt = 20.3 fb ATLAS Preliminary 4l µ = l1τ had 3l 2l0τ had Observed CL s limit Expected CL s Expected CL signal Injected s Expected ± 1 σ Expected ± 2 σ All % CL S limit on µ=σ/σ SM 11

12 and impact on combina3on Ø Clear OH signal produc3on but need stat to reduce uncertainty µ Higgs ATLAS =1.18 ± 0.10 (stat.) ± 7 (exp.sys.)±8(theo.sys.) ATLAS Preliminary m H = GeV H γγ H ZZ* H WW* H ττ VH Vbb H µµ H Zγ tth Overall: µ = ggf: µ = VBF: µ = WH: µ = ZH: µ = Overall: µ = ggf+tth: µ = VBF+VH: µ = Overall: µ = ggf: µ = VBF: µ = VH: µ = Overall: µ = ggf: µ = VBF+VH: µ = Overall: µ = WH: µ = ZH: µ = Overall: µ = Overall: µ = bb: µ = Multilepton: µ = γγ: µ = (GeV) m H Input measurements ± 1σ on µ μ ggf = μ VBF =1.23±0.32 μ VH =0.80±0.36 μ tth =1.81±0.80 ATLAS Preliminary s =7TeV, fb 1 68% CL: 95% CL: s =8TeV,20.3fb 1 m H =125.36GeV Parameter value Ø help to liy the sign ambiguity on κ t thanks to th Generic model allowing Beyond Standard Model in loops: no contraints on κ t from H γγ and H gg loops s = 7 TeV, fb s = 8 TeV, 20.3 fb Signal strength (µ) à Non SM rela3ve sign disfavoured at 1σ 12

13 Conclusions Ø With Run I Data, ATLAS has set limits and measurements on the Higgs boson produced in associa3on with a top quark pair through 3 channels: OHà γγ: µ < 6.7 obs (4.9 exp); µ = (stat.) +0.8 (syst.) OHà bb: µ < 3.4 obs (2.2 exp); µ = 1.5 ±1.1 OHà leptons: µ < 4.7 obs (2.4 exp); µ = All consistent with Standard Model Combined fioed result for OH produc3on is µ=1.81±0.80 σ(oh, 13 TeV)/σ(OH, 8 TeV) ~ 4 ATLAS combinaeon with CMS (µ=2.8±1.0) sell to come Ø The measures are all sta3s3cally limited Ø OH benefits most from space phase opening at 13 TeV à OH very promising for Run II!! Minimum bias W(ln) Z(ll) ZZ t (s-channel) t (t-channel) WH H (ggf) H (VBF) tt ttz tth A(0.5 TeV, ggf+bba) stop pair (0.7 TeV) gluino pair (1.5 TeV) Z' SSM (3 TeV) Q* (4 Tev) QBH (5 TeV) QBH (6 TeV) #TeV#/#8#TeV#inclusive#pp#cross3sec4on#ra4o# ggf VH VBF Marine Kuna - OH ATLAS - PHENO OH

14 GENERAL BACKUP Marine Kuna - OH ATLAS - PHENO

15 Limits Comparison with CMS CMS ATLAS Marine Kuna - OH ATLAS - PHENO

16 Measured Mu Comparison with CMS tth Channel µ = / SM (m H =125.7 GeV) bb l l Same-sign 2l Combined ATLAS (stat) ± ±0.80 (syst) + ATLAS only: 2l+1τ had channel! Marine Kuna - OH ATLAS - PHENO

17 BACKUP TTH GG Marine Kuna - OH ATLAS - PHENO

18 Feynman diagrams th processes OH W _ t _ b g H g t b W Marine Kuna - OH ATLAS - PHENO

19 Yukawa coupling measurement OHà γγ Ø Varia3ons of κ T influence produc3on of OH, th and BR(Hà γγ) Ø limits set on the total Higgs boson produc3on cross sec3on 3mes BR(Hà γγ) with respect to the SM cross sec3on value for different values of κ t Ø 95% CL exclusion below 1.3 and above mes the Yukawa coupling strength in the Standard Model Exclusion limits ProducEon cross seceons NegaEve log likelihood scan Data consistent with SM value κ T =+1 19

20 BACKUP TTH BB Marine Kuna - OH ATLAS - PHENO

21 Processes Marine Kuna - OH ATLAS - PHENO

22 tt+cc Single- lep analysis 4 j, 2 b 4 j, 3 b 4 j, 4 b ATLAS Simulation m H = 125 GeV s = 8 TeV 5 j, 2 b 5 j, 3 b 5 j, 4 b tt+light tt+cc tt+bb tt+v non-tt 6 j, 2 b 6 j, 3 b 6 j, 4 b Single lepton ATLAS Simulation Single lepton s = 8 TeV, 20.3 fb = 125 GeV B S / B S / B S / j, 2 b S/B < 0.1% HT 5 j, 2 b S/B = 0.1% HT 6 j, 2 b S/B = 0.2% HT B S / B S / B S / j, 3 b S/B = 0.2% NN 5 j, 3 b S/B = 0.4% NN (HF- LF) 6 j, 3 b S/B = 1.0% m H B S / B S / B S / NN[ME] 0.5 tt+light 4 j, 4 b S/B = 1.4% NN 5 j, 4 b S/B = 2.5% NN 6 j, 4 b S/B = 4.0% NN[ME] non-tt Marine Kuna - OH ATLAS - PHENO

23 Di- lep analysis 2 j, 2 b ATLAS Simulation m H = 125 GeV s = 8 TeV 3 j, 2 b 3 j, 3 b tt+light tt+cc tt+bb tt+v non-tt 4 j, 2 b 4 j, 3 b 4 j, 4 b Dilepton ATLAS Simulation Dilepton s = 8 TeV, 20.3 fb = 125 GeV S / B S / B j, 2 b S/B < 0.1% j, 2 b S/B = 0.1% HT HT S / B j, 3 b S/B = 0.6% NN m H B S / j, 2 b S/B = 0.3% HT B S / j, 3 b S/B = 1.5% NN S / B j, 4 b S/B = 5.9% NN Marine Kuna - OH ATLAS - PHENO 2015

24 Results Dilepton Lepton+jets Combination ATLAS tth (H bb) s=8 TeV, 20.3 fb Expected ± 1σ Expected ± 2σ Observed Injected signal (µ=1) % CL limit on σ/σ SM at m H =125 GeV Dilepton Lepton+jets Combination tot. stat. ATLAS tth (H bb ) Best fit µ=σ/σ SM s=8 TeV, 20.3 fb ( tot ) ( stat ) 2.8 ± 2.0 ( 1.4 ) 1.2 ± 1.3 ( 0.8 ) 1.5 ± 1.1 ( 0.7 ) for m H =125 GeV Marine Kuna - OH ATLAS - PHENO

25 Ranking Events / ATLAS 5 10 Data tth (µ =1.5) fit tth (µ =3.4) 95% excl. Bkgd tt+bb normalisation jet energy scale 1 tt+cc normalisation tt+bb renormalisation scale choice m bb µ ATLAS s = 8 TeV, 20.3 fb, m =125 GeV H Data / Bkgd tth (H bb) s=8 TeV, 20.3 fb Combined Single lepton and Dilepton tth (µ =1.5) + Bkgd. fit tth (µ =3.4) + Bkgd. 95% excl log (S/B) tt+v cross section tt+bb shower recoil scheme jet energy scale 2 light-jet tagging 1 tt+cc tt p reweighting T b-jet tagging 1 tt+cc top p reweighting T tt+bb renormalisation scale jet energy scale 3 light-jet tagging 2 tt+bb PDF (MSTW) (θ - θ 0 )/ θ Marine 10 Post-fit Impact on µ Kuna - OH ATLAS - PHENO Pull Pre-fit Impact on µ

26 NN entries lep+jets Second Fox- Wolfram moment of jets and leptons Marine Kuna - OH ATLAS - PHENO

27 NN entries lep- lep Marine Kuna - OH ATLAS - PHENO

28 BACKUP TTH LEPTONS Marine Kuna - OH ATLAS - PHENO

29 Processes g g b t H t W + Z 0 Z 0 W b l ν l b l + ν l l + l q q g g t H t W + W + W W b q ν l b l ν l q l + ν l l q g t W + q q b q b q H W + q g l t W + q τ had + g t W + q τ had + g t W W ν l b l g ν l H t τ + τ W ν τ τhad ν τ b l ν l g H t τ + τ W ν τ l ν l ν τ b l ν l Marine Kuna - OH ATLAS - PHENO

30 Signal and Backgrounds : 8 TeV b : reducible, data- driven es3mates, but abundant (~10 8 TeV) ν l l + ν l g g t t W + H τ + τ W l + l + ν l ν τ τ h ν τ q - : same signature thus irreducible, have to manage theory uncertain3es ν l l Z q q q b W q b ν l b W + l + Marine Kuna - OH ATLAS - PHENO ν l l +

31 CutFlow Marine Kuna - OH ATLAS - PHENO

32 Signal Regions Events s = 8 TeV, 20.3 fb ATLAS Preliminary 2l0 Non-Prompt had category Charge misid tth(125) Data 2012 Rare VV ttz ttw Events s = 8 TeV, 20.3 fb ATLAS Preliminary 3l category ttw Non-Prompt tth(125) Data 2012 Rare VV ttz Number of jets Number of jets Events 4 3 s = 8 TeV, 20.3 fb ATLAS Preliminary 2l1 ttw had category Non-Prompt tth(125) Data 2012 Rare VV ttz Events 4 3 s = 8 TeV, 20.3 fb ATLAS Preliminary 4l category ttw Non-Prompt tth(125) Data 2012 Rare VV ttz Events 16 s = 8 TeV, 20.3 fb ATLAS Preliminary Data l2 had category ttw tt Rare VV tth(125) ttz Number of jets Marine Kuna - OH ATLAS - PHENO Number 2015 of jets 32 Number of jets 2 0

33 Valida3on Regions Events 40 s = 8 TeV, 20.3 fb t t Z VR Data ATLAS Preliminary ttw Rare Non-Prompt VV 30 tth(125) ttz Events 35 s = 8 TeV, 20.3 fb t t W VR Data 2012 ATLAS Preliminary Non-Prompt Rare Charge misid tth(125) VV ttz ttw Data / Bkg Number of jets Data / Bkg Number of jets Marine Kuna - OH ATLAS - PHENO

34 Signal strength CMS µ = (ττ) Marine Kuna - OH ATLAS - PHENO

35 Limits 1l2τ had s = 8 TeV, L dt = 20.3 fb 4l ATLAS Preliminary 2l1τ had 3l 2l0τ had Observed CL s limit Expected CL s Expected CL signal Injected s Expected ± 1 σ Expected ± 2 σ All % CL S limit on µ=σ/σ SM Marine Kuna - OH ATLAS - PHENO

36 Event display 2l τ had Marine Kuna - OH ATLAS - PHENO

37 Event display 2l τ had Marine Kuna - OH ATLAS - PHENO

38 Event display 1l2τhad Marine Kuna - OH ATLAS - PHENO

39 BACKUP COMBINATION Marine Kuna - OH ATLAS - PHENO

40 ATLAS Preliminary m H = GeV H γγ H ZZ* H WW* H ττ VH Vbb H µµ H Zγ tth Overall: µ = 1.17 ggf: µ = 1.32 VBF: µ = 0.8 WH: µ = ZH: µ = 0.1 Overall: µ = 1.44 ggf+tth: µ = 1.7 VBF+VH: µ = 0.3 Overall: µ = 1.16 ggf: µ = 0.98 VBF: µ = 1.28 VH: µ = 3.0 Overall: µ = 1.43 ggf: µ = 2.0 VBF+VH: µ = 1.24 Overall: µ = WH: µ = 1.1 ZH: µ = 5 Overall: µ = -0.7 Overall: µ = bb: µ = Multilepton: µ = 2.1 γγ: µ = (GeV) m H Input measurements ± 1σ on µ Decays and produc3on μ ggf = μ VBF =1.23±0.32 μ VH =0.80±0.36 μ tth =1.81±0.80 ATLAS Preliminary s =7TeV, fb 1 68% CL: 95% CL: s =8TeV,20.3fb 1 m H =125.36GeV Parameter value s = 7 TeV, fb s = 8 TeV, 20.3 fb Signal strength Marine Kuna (µ) - OH ATLAS - PHENO

41 Summary of channels entering combina3on Marine Kuna - OH ATLAS - PHENO

42 κ T =- 1 tests If resolved Hà γγ loop or not Marine Kuna - OH ATLAS - PHENO

43 and impact on combina3on Ø Key for Higgs to top quark Yukawa coupling κ t highest produc3on mode signal strength Production process ggf VBF VH 0.93 ± 0.39 tth 1.62 ± 0.78 Signal strength µ at m H = GeV p p s = 8 TeV Combined s = 7 and 8 TeV i i h h i h i h i ± ± ± 0.80 h h i h i h i help to liy the sign ambiguity on κ t thanks to th Generic model allowing Beyond Standard Model in loops: no contraints on κ t from H γγ and H gg loops κ 2 X = Γ H X SM Γ H X but need stat to reduce uncertainty ATLAS Preliminary m H = GeV H γγ H ZZ* H WW* H ττ VH Vbb H µµ H Zγ tth (GeV) m H Overall: µ = ggf: µ = VBF: µ = WH: µ = ZH: µ = Overall: µ = ggf+tth: µ = VBF+VH: µ = Overall: µ = ggf: µ = VBF: µ = VH: µ = Overall: µ = ggf: µ = VBF+VH: µ = Overall: µ = WH: µ = ZH: µ = Overall: µ = Overall: µ = bb: µ = Multilepton: µ = γγ: µ = Input measurements ± 1σ on µ à Non SM excluded at 1σ s = 7 TeV, fb s = 8 TeV, 20.3 fb Signal strength (µ)

44 Summary of the talk Ø Title: Search for Higgs Bosons produced in associa3on with top quarks with the ATLAS detector Ayer the discovery of a Higgs boson, the direct observa3on of the coupling of this par3cle to top quarks is of par3cular importance. In this talk, a review of the latest ATLAS results on the search for the Higgs boson produced in associa3on with top quarks will be presented. Marine Kuna - OH ATLAS - PHENO

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

[ ] Search for tth and th production (not including H bb) at the LHC. !!!!! Top2015 Ischia. Josh McFayden

[ ] Search for tth and th production (not including H bb) at the LHC. !!!!! Top2015 Ischia. Josh McFayden Search for tth and th production (not including H bb) at the LHC [ ] Josh McFayden on behalf of the ATLAS and CMS collaborations Top Ischia 7/9/ Search for tth and th production (not including H bb) at

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

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

Observation of the Higgs boson production in association with top quarks

Observation of the Higgs boson production in association with top quarks Observation of the Higgs boson production in association with top quarks International School of Subnuclear Physics (56 th course), Erice (Sicily) - Italy María Moreno Llácer, CERN 15/6/18 María Moreno

More information

Georges Aad For the ATLAS and CMS Collaboration CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France

Georges Aad For the ATLAS and CMS Collaboration CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France Georges Aad For the ATLAS and CMS Collaboration CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France 5th Large Hadron Collider Physics Conference May 2017, Shanghai Jiao Tong University, Shanghai

More information

Measurements of Fermionic Couplings of the Standard Model Higgs Boson using the bb, ττ and µµ Decay Channels with the ATLAS Detector

Measurements of Fermionic Couplings of the Standard Model Higgs Boson using the bb, ττ and µµ Decay Channels with the ATLAS Detector Measurements of Fermionic Couplings of the Standard Model Higgs Boson using the bb, ττ and µµ Decay Channels with the ATLAS Detector International Europhysics Conference on High Energy Physics Venice,

More information

The Higgs boson discovery. Kern-und Teilchenphysik II Prof. Nicola Serra Dr. Annapaola de Cosa Dr. Marcin Chrzaszcz

The Higgs boson discovery. Kern-und Teilchenphysik II Prof. Nicola Serra Dr. Annapaola de Cosa Dr. Marcin Chrzaszcz The Higgs boson discovery Kern-und Teilchenphysik II Prof. Nicola Serra Dr. Annapaola de Cosa Dr. Marcin Chrzaszcz Higgs production at the LHC g H VBF (Vector Boson Fusion) g gg fusion q 2 W/Z q 0 2 H

More information

ATLAS+CMS Higgs run 1 Combinations

ATLAS+CMS Higgs run 1 Combinations ATLAS+CMS Higgs run 1 Combinations Paolo Francavilla, on behalf of the ATLAS and CMS collaborations 7th Higgs Hunting 2016 August 31 - September 2, LPNHE Paris, France 1 Outline Higgs boson mass measurement

More information

Search for the Higgs boson in fermionic channels using the CMS detector

Search for the Higgs boson in fermionic channels using the CMS detector Search for the Higgs boson in fermionic channels using the CMS detector Centre for Cosmology, Particle Physics and Phenomenology (CP3) Université catholique de Louvain Chemin du Cyclotron, 2 B-1348, Louvain-la-Neuve

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

Kirill Prokofiev (NYU)

Kirill Prokofiev (NYU) Measurements of spin and parity of the new boson in ATLAS Kirill Prokofiev (NYU) Outline Present spin results Short term plans Long term plans page 2 Introduc>on ATLAS and CMS have observed a new Higgs-

More information

ATLAS Di-fermion Results. Koji Nakamura (KEK) on behalf of ATLAS Collaboration

ATLAS Di-fermion Results. Koji Nakamura (KEK) on behalf of ATLAS Collaboration ATLAS Di-fermion Results Koji Nakamura (KEK) on behalf of ATLAS Collaboration 30th July, 2015 Higgs 2015 1 Motivation Higgs boson has been observed by Bosonic decay channels (i.e. γγ,zz,ww) Loop process

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

Higgs couplings and mass measurements with ATLAS. Krisztian Peters CERN On behalf of the ATLAS Collaboration

Higgs couplings and mass measurements with ATLAS. Krisztian Peters CERN On behalf of the ATLAS Collaboration Higgs couplings and mass measurements with ATLAS CERN On behalf of the ATLAS Collaboration July observation: qualitative picture A single state observed around ~125 GeV Qualitatively all observations consistent

More information

Evidence for Higgs Boson Decays to a Pair of τ-leptons

Evidence for Higgs Boson Decays to a Pair of τ-leptons Evidence for Higgs Boson Decays to a Pair of τ-leptons ET miss = 119 GeV μ (pt=6 GeV) τhad (pt=96 GeV) mττ =19 GeV Nils Ruthmann mjj =65 GeV Nils Ruthmann (Universität Freiburg) On Behalf of the ATLAS

More information

D0 Higgs Results and Tevatron Higgs Combination

D0 Higgs Results and Tevatron Higgs Combination D Higgs Results and Tevatron Higgs Combination Graham W. Wilson University of Kansas July 3rd On behalf of the CDF and D collaborations Graham W. Wilson (University of Kansas) BEACH, Wichita July 3rd /

More information

LHC Run1 Higgs Results. Quentin Buat - Simon Fraser University On behalf of the ATLAS and CMS collaborations

LHC Run1 Higgs Results. Quentin Buat - Simon Fraser University On behalf of the ATLAS and CMS collaborations LHC Run1 Higgs Results Quentin Buat - Simon Fraser University On behalf of the ATLAS and CMS collaborations Rencontres de Moriond, QCD session - March 24th, 216 1 Introduction During LHC Run1, ATLAS and

More information

Identification of the Higgs boson produced in association with top quark pairs in proton-proton

Identification of the Higgs boson produced in association with top quark pairs in proton-proton Identification of the Higgs boson produced in association with top quark pairs in proton-proton collision: an analysis of the final state containing three leptons with the ATLAS detector Valentina Vecchio,

More information

ATLAS NOTE ATLAS-CONF th March 2015

ATLAS NOTE ATLAS-CONF th March 2015 ATLAS NOTE ATLAS-CONF-215-7 18th March 215 Measurements of the Higgs boson production and decay rates and coupling strengths using pp collision data at s = 7 and 8 TeV in the ATLAS experiment The ATLAS

More information

Review of Standard Model Higgs results at the ATLAS experiment

Review of Standard Model Higgs results at the ATLAS experiment Journal of Physics: Conference Series PAPER OPEN ACCESS Review of Standard Model Higgs results at the ATLAS experiment To cite this article: Alessandro Calandri and ATLAS Collaboration 7 J. Phys.: Conf.

More information

Overview of the Higgs boson property studies at the LHC

Overview of the Higgs boson property studies at the LHC Overview of the Higgs boson property studies at the LHC Giada Mancini, a, Roberto Covarelli b a LNF-INFN and University of Roma Tor Vergata, b INFN and University of Torino E-mail: giada.mancini@lnf.infn.it,

More information

Combination of Higgs boson searches at ATLAS

Combination of Higgs boson searches at ATLAS Combination of Higgs boson searches at ATLAS Second MCTP Spring Symposium on Higgs Boson Physics, University of Michigan 16 th -20 th April 2012 Gemma Wooden, University of Michigan On behalf of the ATLAS

More information

Measurements of the Higgs Boson at the LHC and Tevatron

Measurements of the Higgs Boson at the LHC and Tevatron Measurements of the Higgs Boson at the LHC and Tevatron Somnath Choudhury (for the ATLAS, CMS, DØ and CDF collaborations) 44 th International Symposium on Multiparticle Dynamics 8 12 September 2014, Bologna

More information

Higgs Production at LHC

Higgs Production at LHC Higgs Production at LHC Vittorio Del Duca INFN LNF WONP-NURT La Habana 5 february 2013 CERN North Jura ATLAS Sketch of LHC North Ring 26,6 Km long and 3,8 m of diameter, made of 8 arches connected by 8

More information

HIGGS STUDIES IN ATLAS AND CMS

HIGGS STUDIES IN ATLAS AND CMS HIGGS STUDIES IN ATLAS AND CMS Nicola De Filippis Politecnico & INFN, Bari and LPC-FNAL, Batavia On behalf of the ATLAS and CMS collaborations N. De Filippis Aug. 31 - Sept. 9, 2018 1 Outline SM Higgs

More information

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

Latest results on the SM Higgs boson in the WW decay channel using the ATLAS detector ATLAS-CONF Latest results on the SM iggs boson in the WW decay channel using the ATLAS detector ATLAS-CONF-6- C. Bertella C. Bertella Second China LC Physics Workshop: CLCP 6 7-December 6 WW lνlν WW channel well-suited

More information

Higgs Boson Physics at the Tevatron

Higgs Boson Physics at the Tevatron Higgs Boson Physics at the Tevatron Koji Sato On Behalf of CDF and D0 Collaborations Windows on the Universe Qui Nhon, August 14, 2013 1 Tevatron Run II p p collisions at s = 1.96 TeV (1.8 TeV in Run I).

More information

Discovery potential of the SM Higgs with ATLAS

Discovery potential of the SM Higgs with ATLAS Discovery potential of the SM Higgs with P. Fleischmann On behalf of the Collaboration st October Abstract The discovery potential of the Standard Model Higgs boson with the experiment at the Large Hadron

More information

arxiv: v1 [hep-ex] 12 Oct 2018

arxiv: v1 [hep-ex] 12 Oct 2018 First observation of the tth process at CMS arxiv:1810.05715v1 [hep-ex] 12 Oct 2018 Kirill Skovpen (on behalf of the CMS Collaboration) Inter-University Institute for High Energies, Vrije Universiteit

More information

The Tevatron s Search for High Mass Higgs Bosons

The 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 information

Search for top squark pair production and decay in four bodies, with two leptons in the final state, at the ATLAS Experiment with LHC Run2 data

Search for top squark pair production and decay in four bodies, with two leptons in the final state, at the ATLAS Experiment with LHC Run2 data Search for top squark pair production and decay in four bodies, with two leptons in the final state, at the ATLAS Experiment with LHC Run data Marilea Reale INFN Lecce and Università del Salento (IT) E-mail:

More information

Combined Higgs Results

Combined Higgs Results Chapter 2 Combined Higgs Results This chapter presents the combined ATLAS search for the Standard Model Higgs boson. The analysis has been performed using 4.7 fb of s = 7 TeV data collected in 2, and 5.8

More information

Search for Invisible Decay of Higgs boson at LHC

Search for Invisible Decay of Higgs boson at LHC Search for Invisible Decay of Higgs boson at LHC Kajari Mazumdar Tata Institute of Fundamental Research Mumbai DHEP seminar, TIFR, Mumbai 22.4.2014 Plan of the talk Preliminaries Status of measurements

More information

Higgs boson measurements at ATLAS

Higgs boson measurements at ATLAS Higgs boson measurements at On behalf of the Collaboration Oxford University E-mail: chris.hays@physics.ox.ac.uk A comprehensive set of Higgs boson measurements has been performed in pp collisions produced

More information

ATLAS Discovery Potential of the Standard Model Higgs Boson

ATLAS Discovery Potential of the Standard Model Higgs Boson ATLAS Discovery Potential of the Standard Model Higgs Boson Christian Weiser University of Freiburg (on behalf of the ATLAS Collaboration) 14th Lomonosov Conference on Elementary Particle Physics Moscow,

More information

} Very nice new results on limits

} Very nice new results on limits The Higgs Boson : Latest Measurements and Perspectives Thomas Muller (KIT), on behalf of the ATLAS and CMS Collaborations Outline: Introduction Bosonic decay channels (γγ, ZZ, WW) Fermionic decays (ττ,

More information

Higgs search in WW * and ZZ *

Higgs search in WW * and ZZ * Higgs search in WW * and ZZ * Emanuele Di Marco on behalf of CMS collaboration La Sapienza Università di Roma & INFN Roma1 July, 29 2011 1 Higgs production at LHC gluon fusion (gg H) gg H is the dominant

More information

Searches for New Phenomena in Events with Multiple Leptons with the ATLAS Detector

Searches 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 information

Search for a SM Higgs Boson in semi-leptonic di-tau final states with ATLAS at the LHC

Search for a SM Higgs Boson in semi-leptonic di-tau final states with ATLAS at the LHC Search for a SM Higgs Boson in semi-leptonic di-tau final states with ATLAS at the LHC ET miss = 9 GeV μ (pt=63 GeV) τhad (pt=96 GeV) mττ =9 GeV Nils Ruthmann mjj =65 GeV Nils Ruthmann Universität Freiburg

More information

Searches for gaugino produc1on with the ATLAS detector

Searches for gaugino produc1on with the ATLAS detector Searches for gaugino produc1on with the ATLAS detector SEARCH 2012 University of Maryland, USA (Stockholm U.) on behalf of the ATLAS Collabora1on Search 2012 March 18 th 2012 1 Gaugino Produc1on Signals

More information

Higgs Property Measurement with ATLAS

Higgs Property Measurement with ATLAS Higgs Property Measurement with ATLAS Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University Hadron Collider Physics Symposium HCP 2012, Kyoto University, Japan November 12-16, 2012 Observation

More information

Higgs Coupling Measurements!

Higgs Coupling Measurements! Status, prospects, and interplay with searches for physics BSM Seminar University of California - Irvine April 23rd, 2014 Introduction Fantastic progress since discovery July 2012 Observation in three

More information

Study of Higgs boson production in the WW decay channel at the LHC

Study of Higgs boson production in the WW decay channel at the LHC Study of iggs boson production in the decay channel at the LC Tatjana Lenz on behalf of the and CMS collaborations.8.3 Rencontres du Vietnam Introduction n th July - the discovery of a new particle n and

More information

Title Text. ATLAS Higgs Boson Discovery Potential

Title Text. ATLAS Higgs Boson Discovery Potential Title Text ATLAS Higgs Boson Discovery Potential Isabelle Wingerter-Seez - LAPP - Annecy isabelle.wingerter@lapp.in2p3.fr Corfu Summer Institute September 2009 1 Title Text ATLAS Standard Model Higgs Boson

More information

Searches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector

Searches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector Searches for electroweak production of supersymmetric gauginos and sleptons with the ATLAS detector Christopher Bock on behalf of the ATLAS Collaboration SUSY5 - August 7, 5 Introduction Outline Introduction

More information

CMS Higgs Results Adi Bornheim Caltech

CMS Higgs Results Adi Bornheim Caltech CMS Higgs Results Adi Bornheim Caltech 06.04.2014 1 A brief history of recent times W & Z Boson t-quark H Boson 1964 1974 1984 1994 2004 2014 Peter Higgs This talk : Summary of 29 CMS publications and

More information

Higgs Boson at the CMS experiment

Higgs Boson at the CMS experiment 16 th Lomonosov Conference on Elementary Particle Physics 22 28 August 2013, Moscow (Russia) Higgs Boson at the CMS experiment Somnath Choudhury (for the CMS collaboration) 5.1 fb -1 @ 7 TeV + 5.3 fb -1

More information

Search for a new spin-zero resonance in diboson channels at 13 TeV with the CMS experiment

Search for a new spin-zero resonance in diboson channels at 13 TeV with the CMS experiment Search for a new spin-zero resonance in diboson channels at 3 TeV with the experiment Universite Catholique de Louvain (UCL) (BE) E-mail: alessio.magitteri@cern.ch On behalf of the Collaboration Searches

More information

Search for Standard Model Scalar Boson Decaying to Fermions at the LHC

Search for Standard Model Scalar Boson Decaying to Fermions at the LHC Search for Standard Model Scalar Boson Decaying to Fermions at the LC on behalf of the ATLAS and CMS collaborations Rencontres de Moriond QCD and igh Energy Interactions March 9 th 6 th, 3 95% CL limit

More information

Higgs Boson Searches at ATLAS

Higgs Boson Searches at ATLAS Higgs Boson Searches at ATLAS Jianming Qian University of Michigan October 5, 2011 Maryland/John Hopkins Joint Seminar, October 5, 2011 Jianming Qian (University of Michigan) 1 Standard Model Standard

More information

Search for the SM Higgs in τ l τ h jj Final States: Production Modes and Background Modeling

Search for the SM Higgs in τ l τ h jj Final States: Production Modes and Background Modeling Search for the SM Higgs in τ l τ h jj Final States: Production Modes and Background Modeling Ian Howley on behalf of the DØ Collaboration APS April Meeting, Atlanta GA March 30, 2012 I. Howley (UT Arlington)

More information

Iden%fica%on and energy calibra%on of hadronically decaying tau leptons with the ATLAS experiment.

Iden%fica%on and energy calibra%on of hadronically decaying tau leptons with the ATLAS experiment. Iden%fica%on and energy calibra%on of hadronically decaying tau leptons with the ATLAS experiment. Almut Pingel Niels Bohr Ins3tute on behalf of the ALTAS collabora3on ICHEP, Valencia (Spain) 3 July 214

More information

Higgs Searches at CMS

Higgs Searches at CMS Higgs Searches at CMS Ashok Kumar Department of Physics and Astrophysics University of Delhi 110007 Delhi, India 1 Introduction A search for the Higgs boson in the Standard Model (SM) and the Beyond Standard

More information

Tutorial 8: Discovery of the Higgs boson

Tutorial 8: Discovery of the Higgs boson Tutorial 8: Discovery of the Higgs boson Dr. M Flowerdew May 6, 2014 1 Introduction From its inception in the 1960 s, the Standard Model was quickly established, but it took about 50 years for all of the

More information

Measurements of the Higgs Boson Couplings and Other Properties at the LHC

Measurements of the Higgs Boson Couplings and Other Properties at the LHC Measurements of the Higgs Boson Couplings and Other Properties at the LHC Marcello Fanti (on behalf of the ATLAS and CMS collaborations) University of Milano and INFN M. Fanti (Physics Dep., UniMi) Higgs

More information

How to find a Higgs boson. Jonathan Hays QMUL 12 th October 2012

How to find a Higgs boson. Jonathan Hays QMUL 12 th October 2012 How to find a Higgs boson Jonathan Hays QMUL 12 th October 2012 Outline Introducing the scalar boson Experimental overview Where and how to search Higgs properties Prospects and summary 12/10/2012 2 The

More information

Searches for SM H ττ at the LHC

Searches for SM H ττ at the LHC Searches for SM H ττ at the LHC M.Bachtis University of Wisconsin-Madison On behalf of the ATLAS and CMS Collaborations arxiv:1202.4083, ATLAS-CONF-2012-014 CMS PAS HIG-12-006, HIG-12-007 Introduction

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

in Section The H ZZ 4l channel

in 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 information

Un-ki Yang. Seoul National University. WIN 2015, June 8-13, 2015, MPIK Heidelberg, On behalf of the ATLAS and CMS collaborations

Un-ki Yang. Seoul National University. WIN 2015, June 8-13, 2015, MPIK Heidelberg, On behalf of the ATLAS and CMS collaborations Un-ki Yang Seoul National University On behalf of the ATLAS and CMS collaborations! WIN 2015, June 8-13, 2015, MPIK Heidelberg,! ! Small neutrino mass " heavy neutrino (N R ) by SeaSaw! Type I : weak-singlet

More information

Higgs Boson Measurements from ATLAS and CMS. Giacinto Piacquadio on behalf of the ATLAS and CMS Collaborations. ICHEP Seoul July 10th, 2018

Higgs Boson Measurements from ATLAS and CMS. Giacinto Piacquadio on behalf of the ATLAS and CMS Collaborations. ICHEP Seoul July 10th, 2018 Higgs Boson Measurements from ATLAS and CMS Giacinto Piacquadio on behalf of the ATLAS and CMS Collaborations ICHEP 2018 - Seoul July th, 2018 1 The Higgs boson in the SM The Higgs boson discovery in 2012

More information

Higgs Prospects for future (HL)LHC runs

Higgs Prospects for future (HL)LHC runs ATLAS & CMS Higgs Prospects for future (HL)LHC runs L 3000 fb-1 Rencontres du Vietnam 2014 O. Arnaez CERN tme 1/21 Introduction Search and discovery of the Brout-Englert-HiggsGuralnik-Hagen-Kibble boson,

More information

Higgs Results from ATLAS

Higgs Results from ATLAS Higgs Results from ATLAS Rosy Nikolaidou CEA Saclay On behalf of ATLAS collaboration Rencontres de Moriond QCD and High Energy Interac7ons La Thuile, March 5th - April st, 7 Introduction & Outline Ø After

More information

SUSY Phenomenology & Experimental searches

SUSY Phenomenology & Experimental searches SUSY Phenomenology & Experimental searches Alex Tapper Slides available at: http://www.hep.ph.ic.ac.uk/tapper/lecture.html Reminder Supersymmetry is a theory which postulates a new symmetry between fermions

More information

Review of Higgs results at LHC (ATLAS and CMS results)

Review of Higgs results at LHC (ATLAS and CMS results) Review of Higgs results at LHC (ATLAS and CMS results) Università degli Studi di Genova and INFN, Genova, Italy E-mail: andrea.favareto@ge.infn.it The status of Higgs sector studies at the Large Hadron

More information

Search for the Standard Model Higgs boson decaying to b quark with CMS experiment

Search for the Standard Model Higgs boson decaying to b quark with CMS experiment Search for the Standard Model Higgs boson decaying to b quark with CMS experiment Silvio Donato 1 2 3 4 on behalf of the CMS Collaboration 1 Scuola Normale Superiore, Piazza dei Cavalieri, 7-56126, Pisa,

More information

Searching for the Higgs at the Tevatron

Searching for the Higgs at the Tevatron Searching for the Higgs at the Tevatron 5 th May 2009 Particle Physics Seminar, Oxford Outline Introduction The challenges and analysis strategies Low mass SM Higgs searches High mass SM Higgs searches

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

Beyond the Standard Model Higgs boson searches using the ATLAS etector

Beyond the Standard Model Higgs boson searches using the ATLAS etector EPJ Web of Conferences 95, 47 (5) DOI:.5/ epjconf/ 5947 C Owned by the authors, published by EDP Sciences, 5 Beyond the Standard Model Higgs boson searches using the ATLAS etector I.I. Tsukerman the ATLAS

More information

Higgs searches in CMS

Higgs searches in CMS Higgs searches in CMS Mario Pelliccioni Istituto Nazionale di Fisica Nucleare Torino Miami 2012 17/12/12 Introduction Why do we even bother to look for the Higgs? An Higgs boson naturally emerges from

More information

Higgs Boson in Lepton Decay Modes at the CMS Experiment

Higgs Boson in Lepton Decay Modes at the CMS Experiment Higgs Boson in Lepton Decay Modes at the Experiment Somnath Choudhury 1 for the collaboration 1 DESY - Hamburg, Germany DOI: http://dx.doi.org/1.34/desy-proc-14-4/1 The results on the standard model Higgs

More information

HIGGS Bosons at the LHC

HIGGS Bosons at the LHC ATLAS HIGGS Bosons at the LHC Standard Model Higgs Boson - Search for a light Higgs at the LHC - Vector boson fusion - Comparison to the Tevatron potential Measurement of Higgs boson parameters The MSSM

More information

Search for the Higgs Boson at the LHC. Karl Jakobs Physikalisches Institut Universität Freiburg

Search for the Higgs Boson at the LHC. Karl Jakobs Physikalisches Institut Universität Freiburg Search for the Higgs Boson at the LHC Karl Jakobs Physikalisches Institut Universität Freiburg Outline of the talk:. Introduction, the Higgs boson in the Standard Model. The Standard Model Higgs boson

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

Constraints on the Higgs Width

Constraints on the Higgs Width Constraints on the Higgs Width Andrew Whitbeck (Fermilab) On behalf of the CMS collaboratsion!! Americas Workshop on Linear Colliders May 14, 2014 Results shown are from: CMS-PAS-HIG-14-002 Higgs Properties

More information

SEARCH FOR ASSOCIATED PRODUCTION OF THE HIGGS BOSON IN THE H W W CHANNEL WITH A FULLY LEPTONIC FINAL STATE

SEARCH FOR ASSOCIATED PRODUCTION OF THE HIGGS BOSON IN THE H W W CHANNEL WITH A FULLY LEPTONIC FINAL STATE Vol. 45 (2014) ACTA PHYSICA POLONICA B No 7 SEARCH FOR ASSOCIATED PRODUCTION OF THE HIGGS BOSON IN THE H W W CHANNEL WITH A FULLY LEPTONIC FINAL STATE Valerio Bortolotto on behalf of the ATLAS Collaboration

More information

ATLAS-CONF CMS-PAS-HIG th September 2015

ATLAS-CONF CMS-PAS-HIG th September 2015 ATLAS-CONF-2015-044 CMS-PAS-HIG-15-002 15th September 2015 Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC

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 -08/036 he Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH GENEVA 3, Switzerland 30 April 08 (v4, 08 May 08) Measurement of the

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

Search for BSM Higgs bosons in fermion decay modes with ATLAS

Search for BSM Higgs bosons in fermion decay modes with ATLAS Search for BSM Higgs bosons in fermion decay modes with ATLAS A. Straessner on behalf the ATLAS Collaboration FSP 103 ATLAS CC BY-SA 3.0 LHCP 2017 Shanghai May 15-20, 2017 LHCHXSWG-2015-002 arxiv:1302.7033

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

Dmitri Sidorov Oklahoma State University On behalf of the ATLAS Collaboration DIS2014, 04/28/2014

Dmitri Sidorov Oklahoma State University On behalf of the ATLAS Collaboration DIS2014, 04/28/2014 Dmitri Sidorov Oklahoma State University On behalf of the ATLAS Collaboration DIS4, 4/8/4 Introduc)on We discovered a Standard Model (SM) like Higgs boson at mh=5 GeV. This is not the end of the story.

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

arxiv: v1 [hep-ex] 7 Jan 2019

arxiv: v1 [hep-ex] 7 Jan 2019 Top quarks and exotics at ATLAS and CMS Leonid Serkin on behalf of the ATLAS and CMS Collaborations 1 arxiv:1901.01765v1 [hep-ex] 7 Jan 2019 INFN Gruppo Collegato di Udine, Sezione di Trieste, Udine and

More information

Search for the Standard Model Higgs Boson in H WW lν lν with the ATLAS experiment

Search for the Standard Model Higgs Boson in H WW lν lν with the ATLAS experiment Search for the Standard Model Higgs Boson in H WW lν lν with the ATLAS experiment MCTP Symposium 2012, University of Michigan, Ann Arbor, US Outline SM Higgs Boson production and decay Analysis based on

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 -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

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

Higgs Boson Searches in ATLAS

Higgs Boson Searches in ATLAS Higgs Boson Searches in ATLAS Wolfgang F. Mader Institut für Kern- und Teilchenphysik TU Dresden Fourth fermion generation and single-top production 202 26-28 March 202 Leinsweiler, Pfalz, Germany Wolfgang

More information

SEARCH FOR INVISIBLE DECAY MODES OF THE HIGGS BOSON WITH THE ATLAS DETECTOR

SEARCH FOR INVISIBLE DECAY MODES OF THE HIGGS BOSON WITH THE ATLAS DETECTOR SEARCH FOR INVISIBLE DECAY MODES OF THE HIGGS BOSON WITH THE ATLAS DETECTOR Monica Trovatelli (University of Victoria) on behalf of the ATLAS Collaboration HIGGS INVISIBLE DECAY SEARCHES: WHY? Standard

More information

Taller de Altas Energías Michael Holzbock September 7, LMU Munich

Taller de Altas Energías Michael Holzbock September 7, LMU Munich Search for top squark pair production in final states with two τ leptons, jets, and missing transverse momentum in s = TeV pp-collisions with the ATLAS detector Taller de Altas Energías 6 Michael Holzbock

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

Search for a heavy scalar boson decaying into a pair of Z bosons in the 2l2ν final state in CMS

Search for a heavy scalar boson decaying into a pair of Z bosons in the 2l2ν final state in CMS Search for a heavy scalar boson decaying into a pair of Z bosons in the 2l2ν final state in CMS Li Yuan Beihang University CLHCP 2016 December 18, 2016 1 Outline Introduction Overview Analysis Strategy

More information

New Physics Searches at CMS

New Physics Searches at CMS New Physics Searches at CMS! Higgs Portal Workshop: UMass, Amherst John Paul Chou Rutgers University! Thursday, May st, OUTLINE The space of New Physics searches is vast Nevertheless, I assume most everyone

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

Search for the Standard Model Higgs in WW (lν)(lν)

Search for the Standard Model Higgs in WW (lν)(lν) Search for the Standard Model Higgs in WW (lν)(lν) v l v l Yanyan Gao (Fermilab) February 11, 13 HEP Lunch seminar at University of Chicago The SM Higgs Production and Decays at LHC "(pp! H+X) [pb] The

More information

Evidence for the decay of the SM Higgs Boson to Fermions

Evidence for the decay of the SM Higgs Boson to Fermions Evidence for the decay of the SM Higgs Boson to Fermions A presentation of Steffen Landgraf Advised by Prof. Dr. M. Schumacher University of Freiburg 1 Higgs Boson to Fermions decay 1 Talk outline Introduction

More information

Tevatron 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 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 information

From the Discovery of the Higgs Boson to the Search for Dark Matter -New results from the LHC-

From the Discovery of the Higgs Boson to the Search for Dark Matter -New results from the LHC- From the Discovery of the Higgs Boson to the Search for Dark Matter -New results from the LHC- Karl Jakobs Physikalisches Institut Universität Freiburg / Germany LHC and Data Taking, First look at the

More information

Search for Higgs Bosons at LEP. Haijun Yang University of Michigan, Ann Arbor

Search for Higgs Bosons at LEP. Haijun Yang University of Michigan, Ann Arbor Search for Higgs Bosons at LEP Haijun Yang University of Michigan, Ann Arbor L3 On behalf of the L3 Collaboration American Physical Society Meeting(APS03), Philadelphia April 5-8, 2003 OUTLINE Introduction

More information