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

Similar documents
Evidence for tth production at ATLAS

Recent ATLAS measurements in Higgs to diboson channels

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

Observation of the Higgs boson production in association with top quarks

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

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

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

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

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

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

ATLAS NOTE ATLAS-CONF th March 2015

Higgs search in WW * and ZZ *

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

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

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

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

Understanding the Higgs Boson: Where We Are, Where We re Going, and How To Get There

Searches for new physics at ATLAS using pair production of Higgs bosons. Jahred Adelman

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

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

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

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

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

Review of Standard Model Higgs results at the ATLAS experiment

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

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

The Tevatron s Search for High Mass Higgs Bosons

Perspectives of Higgs measurements at High-Luminosity LHC

Higgs Boson Searches in ATLAS

Bounding the Higgs boson width from off-shell production and decay to ZZ 4l

Higgs Boson Searches at ATLAS

Search for Invisible Decay of Higgs boson at LHC

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

Higgs boson properties (ATLAS and CMS)

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

CMS Higgs Results Adi Bornheim Caltech

t th production at the LHC

Searches for SM H ττ at the LHC

Title Text. ATLAS Higgs Boson Discovery Potential

Higgs Boson at the CMS experiment

Status of ATLAS Higgs Search

arxiv: v1 [hep-ex] 12 Oct 2018

Search for BSM Higgs bosons in fermion decay modes with ATLAS

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

Dimitris Iliadis AUTh, LAPP. On behalf of the ATLAS collaboration. XIIth Quark Confinement and the Hadron Spectrum 29 August 2016, Thessaloniki

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

Combination of Higgs boson searches at ATLAS

Search for Higgs to tt at CMS

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

Searching for the Higgs at the Tevatron

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

Tutorial 8: Discovery of the Higgs boson

Combined Higgs Results

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

ATLAS Discovery Potential of the Standard Model Higgs Boson

Higgs decaying into bosons

Higgs Production at LHC

Beyond the Standard Model Higgs boson searches using the ATLAS etector

ATLAS+CMS Higgs run 1 Combinations

Measurements of the Higgs Boson at the LHC and Tevatron

ATLAS-CONF CMS-PAS-HIG th September 2015

Higgs Results from ATLAS

HIGGS STUDIES IN ATLAS AND CMS

Higgs Coupling Measurements!

Measurement of the Higgs Couplings by Means of an Exclusive Analysis of its Diphoton decay

Multi-Boson Interactions CMS HL-LHC Multi-boson Physics Prospect

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

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

in Section The H ZZ 4l channel

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

CMS Searches for New Physics

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

Overview of the Higgs boson property studies at the LHC

Constraints on Higgs-boson width using H*(125) VV events

tt + X production at ATLAS and CMS

Search for the Standard Model Higgs boson decaying into a WW pair

Future ATLAS Higgs Studies Ben Smart, On behalf of the ATLAS collaboration

Higgs boson measurements at ATLAS

Lepton Flavour Violation at ATLAS & CMS

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

Higgs Searches at CMS

ATLAS+CMS Higgs combination: what have we learned? SM physics: what have we learned?

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

New Physics Searches at CMS

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

Higgs-related SM Measurements at ATLAS

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

Higgs Prospects for future (HL)LHC runs

Studies and Prospects of Higgs searches

Higgs Boson Physics at the Tevatron

Search for the SM Higgs Boson in H γγ with ATLAS

Pedro Teixeira-Dias. Higgs Overview

Higgs searches in CMS

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

Search for Higgs in H WW lνlν

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

Searching for additional Higgs bosons at the CERN Large Hadron Collider

D0 Higgs Results and Tevatron Higgs Combination

WZ di-boson production at CMS

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

Transcription:

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 the LHC Josh McFayden on behalf of the ATLAS and CMS collaborations Top Ischia 7/9/

Introduction Since the Higgs discoveries the focus of experiment has been to measure its properties including its coupling to SM particles. Higgs observed decaying to H γγ, H ZZ* 4l, H WW* lυlυ, evidence for H ττ. The large mass of the top quark implies a top Yukawa coupling ~. There is already sensitivity in to the top-higgs coupling from ggf Higgs production and from the decay to photons via loop interactions: g t t t H H t g t t 3 Josh McFayden Top 7/9/

Introduction Production in association with ttbar would permit a direct measurement of the top-higgs coupling Removing possible BSM effects in the loops. Production in association with a single top quark is sensitive to W-t interference and relative sign of the top-higgs coupling g g t t t H t Tree level interference in all channels and in Hγγ loop for H γγ 4 Josh McFayden Top 7/9/

Analyses covered ATLAS and CMS analyses searching for a Higgs produced in association with top quark pairs (tth) and single top quarks (th) are presented. This talk focuses on searches in decay modes not including H bb In reality this means H γγ, H ZZ*, H WW* and H ττ. Signatures are di-photons, same-sign (SS) di-lepton and multi-lepton final states Higgs BR + Total Uncert - -3-4 bb WW gg cc ZZ Z µµ 3 4 6 7 8 9 3 M H [GeV] LHC HIGGS XS WG 3 H WW =.4 H ττ =.6 H ZZ =.8 H γγ =. t[t]h( γγ): Physics Letters B 74 () -4 t[t]h( leptons): Physics Letters B 749 () 9-4 tth(h all): J. High Energy Phys. 9 (4) 87 th( γγ): HIG4- tth(h leptons): HIG3- th( leptons): HIG4-6 Josh McFayden Top 7/9/

6 Josh McFayden Josh McFayden MC performance Top // 7/9/ H γγ

7 Josh McFayden Top 7/9/ t[t]h γγ Analysis strategy ATLAS and CMS use both s = 7 & 8 TeV datasets for this analysis. ATLAS includes th in the definition of signal whilst CMS has a separate analysis. Two signal regions defined by top decay modes Leptonic and hadronic categories. Use excellent m γγ resolution to extract signal peak from falling continuum background. Background estimated from data using m γγ sidebands. Signal strength, μ, is extracted from fit to m γγ distribution Higgs mass is fixed while μ is allowed to float but is common across the different signal regions.

8 Josh McFayden Top 7/9/ t[t]h γγ Results Dominant systematic uncertainties are: Photon ID Background modelling Jet energy scale Theory & MC modelling Results are consistent with the SM expectation / GeV / GeV 4 3 8 6 4 Background fit µ =.4 ATLAS s = 8 TeV Ldt =.3 fb tth, H γ γ, m H 8 TeV leptonic category =.4 GeV 3 4 6 [GeV] Background fit µ =.4 ATLAS m γ γ s = 8 TeV Ldt =.3 fb tth, H γ γ, m H 8 TeV hadronic category =.4 GeV CMS tth γγ leptonic 6 Bkg fit ±σ ±σ 4 m H =.6GeV 3 s = 8 TeV, L = 9.7 fb 4 6 8 (GeV) 4 3 CMS tth γγ hadronic m γγ s = 8 TeV, L = 9.7fb 6 Bkg fit ±σ ±σ m H =.6GeV 3 4 6 [GeV] m γ γ 4 6 8 (GeV) m γγ

t[t]h γγ tth Interpretation The H γγ observed (exp.) 9%CL upper limits on σ/σsm: ATLAS: 6.7 (4.9 +.6.4) CMS: 7.4 (4.7 +.9.6) The H γγ best-fit tth signal strengths: ATLAS: μtth=.3 +.6.7 CMS: μtth=.7 +.6.8 CMS s = 7 TeV,.-. fb ; s = 8 TeV, 9.39.7 fb ATLAS - s=7 TeV, L dt=4. fb s=8 TeV, L dt=.3 fb γγ bb Expected ± σ Expected ± σ Expected (sig. inj.) Observed Hadronic τ h τ h Combined 9 Leptonic 3 3 9% CL limit on σ tt H /σ tt H SM at m H t Expected (σ t H =) ± t Expected (σ t H =) ± Observed SM signal injected σ σ =.4 GeV 4l 3l Same-Sign l Combination 9% CL limit on σ/σ SM at m H =.6 GeV Josh McFayden Top 7/9/

t[t]h γγ th Interpretation Results can also be interpreted in terms of the scale of the top Yukawa coupling, κ t or C t. At the 9% CL ATLAS exclude κ t <.3 and κ t > 8.. Expectation w.r.t SM Limits constrain BSM models. - -3-4 ATLAS tth, H γ γ s = 8 TeV, m H =.4 GeV SM BR(H γ γ ) BR SM (H γ γ ) σ(tth)/σ SM (tth) σ(th)/σ SM (th) - 4 6 8 κ t th Results: - ATLAS result included in tth search - CMS dedicated search for thq. No events observed: 9%CL upper limit on σ/σsm of 4. for inverted coupling (Ct=). γ ) )(κ t ) γ γ γ σ BR(H σ BR(H 9% CL limit on 3 - ATLAS - / ( GeV)..4.3.. - 4 6 8 κ Top 7/9/ t Josh McFayden CMS Preliminary, L = 9.7 fb at 3 4 6 7 8 Diphoton Mass [GeV] Ldt = 4. fb Ldt =.3 fb s = 7 TeV Observed CL s limit Expected CL s limit ± σ ± σ,, thq (Ct = ) Extra tth (Ct = ) tth () VH () s = 8 TeV s = 8 TeV

Josh McFayden Josh McFayden MC performance Top // 7/9/ H leptons

tth leptons Analysis strategy Final state considered is the following: p p t t H b b W W W W b b W W τ τ l=e,μ Signal regions selection: Common selection: Fit strategy: l SS τhad 4j, b 4j, btight bloose l SS τhad 4j, b 3l 4j, b 3j, b j, btight bloose 4l j, b, Zenriched/deprived Njets τhad l, 3j, b Within H bb framework m(ll) cuts veto for low mass resonances & Z candidates miss ET /HT - LD cut to remove Z+jets Yield in SRs ATLAS signal category by Higgs decay mode (CMS ~same) Shape: BDT bins & Njets (lτhad split SRs by Njets & l-flav) (Njets is used in 4l-only) Josh McFayden Top 7/9/

tth leptons Backgrounds Dominant backgrounds can be split into two categories Irreducible: ttv, diboson(+bjet) Use validation regions to validate MC with data Reducible: non-prompt leptons Use control regions with loosened isolation requirements to extrapolate to signal region 4 ± µ ± CMS tth, e channel s = 8 TeV, L = 9.6 fb ttw/z/h ttγ Others Non Pr 3 3 3 3 4 6 7 8 9 Trailing lepton p T (GeV) Josh McFayden Top 7/9/

tth leptons Results Dominant systematic uncertainties: 4 Non-prompt lepton background estimation Theory & MC modelling Jet energy scale Signal strength extraction from fit to: ATLAS Charge misid Rare 8 6 4 4 8 6 4 s = 8 TeV,.3 fb lτ had category signal region ATLAS s = 8 TeV,.3 fb 8 3l category 6 yields Shape of 4 BDT & N jet distribution(s) Total unc. tth() X.4 3 4 6 7 8 Number of jets ttw Total unc. tth() X.4 VV ttz ttw Rare 3 4 6 7 8 Number of jets VV ttz tth ttw ttz/γ* ttγ WZ Others Non Pr Ch misid tth x 3 tth ttw 3 ttz/γ* ttγ WZ Others Fakes tth x 3 ± µ ± CMS tth, e channel s = 8 TeV, L = 9. fb -.8 -.6 -.4 -...4.6.8 BDT output CMS tth, 3l channel s = 8 TeV, L = 9. fb -.8 -.6 -.4 -...4.6 BDT output Josh McFayden Top 7/9/

tth leptons Limits on σ/σsm The results are compatible with the SM expectation, although an excess is observed by both experiments. l SS and 3l categories are the most sensitive The H leptons observed (exp.) 9%CL upper limits on σ/σ SM : ATLAS - 4l: 8 ( +8-4) CMS - 4l: 6.8 (8.8 +. -.) 3l: 6.8 (3.8 +.9.) 3l: 7. (4. +..3) lτhad: 6.7 (3.9 +.8.) l: 9. (3.4 +.6.) lτ had 4l ATLAS s = 8 TeV,.3 fb γγ bb CMS s = 7 TeV,.-. fb ; s = 8 TeV, 9.39.7 fb Expected ± σ Expected ± σ Expected (sig. inj.) Observed lτ had 3l lτ had All Observed CL s limit Expected CL s Expected CL signal Injected s Expected ± σ Expected ± σ τ h τ h 4l 3l Same-Sign l Combination 9% CL S limit on µ=σ/σ SM 9% CL limit on σ/σ SM at m H =.6 GeV Josh McFayden Top 7/9/

tth leptons Signal strength The results are compatible with the SM expectation, although an excess is observed by both experiments. l SS and 3l categories are the most sensitive. The H leptons observed best-fit signal strengths: ATLAS - 4l:.8 +6.9 -. CMS - 4l: -4.7 +..3 3l:.8 +..8 3l: 3. +.4 -. lτhad:.8 +..9 CMS l:.3 +. s.8 γγ = 7 TeV,.-. fb ; s = 8 TeV, 9.39.7 fb bb τ h τ h CMS s = 7 TeV,.-. fb ; s = 8 TeV, 9.39.7 fb τ h τ h 4l 4l 3l 3l Same-Sign l Same-Sign l Combination 6 Combination -8-6 -4-4 6 8 Best fit σ/σ SM at m H =.6 GeV -8-6 -4-4 6 8 Josh McFayden Top 7/9/

+. ggf+tth: µ =.7.36 -.4 +.6 VBF+VH: µ =.3 -.9.36 tth All +.4 tth combination results Overall: µ =.6.36 -. H WW* +.9 ggf: µ =.98.36 -.6 +. The combined VBF: µ =.8.36 observed (exp.) 9%CL upper limits on σ/σ -.47 SM : = 3. +.6 VH: µ.3.36 ATLAS: 3. (.4) +.43 H ττ ATLAS Overall: µ =.43 Individual H Zγ +4. Overall: analysis µ =.7 s = 7 TeV, 4.-4.7 fb μ ggf =.3 +.3. s = 8 TeV,.3 fb.36 -.37 +. ggf: µ =..36. The +.9 VBF+VH: combined µ =.4 observed best-fit signal strengths: -.4.36 =. +.4 Overall: µ.36 -.4 VH Vbb ATLAS: μ=.8 +.8.8 CMS: μ=.9 +.8 -.94 +.6 H µµ tth WH: µ =. ZH: µ =. Overall: µ = -.7 -.6 +. -.49 +3.7-3.7-4.3 +. bb: µ =.. +.4 Multilepton: µ =. γγ: µ =.3 μ VH =.8±.36. +.6.7 μ VBF =.3±.3.. (GeV) m H.4 ATLAS 68% CL: 9% CL: ATLAS 68% CL: 9% CL: Input measurements ± σ on µ s =7TeV,4. 4.7fb s =8TeV,.3fb 4 Signal strength (µ) s =7TeV,4. 4.7fb s =8TeV,.3fb µ µ γγ bb τ h τ h 4l 3l Same-Sign l ggh Combination CMS: 4. (.7 +.8 -.) CMS =.8 +.9 -.6 +.37 =.6-8 -6-4 - 4 6 8 VBF -.34 +.38 µ =.9 VH -.36 CMS CMS s = 7 TeV,.-. fb ; s = 8 TeV, 9.39.7 fb 9.7 fb (8 TeV) +. fb (7 TeV) 68% CL 9% CL Best fit σ/σ SM at m H =.6 GeV 9.7 fb (8 TeV) +. fb (7 TeV) 68% CL 9% CL 7 μ tth =.8±.8 μ ggf =.3 +.3. μ VBF =.3±.3 μ VH =.8±.36 m H =.36GeV... 3 Signal strength (μ).36 hep-ph 7.448 µ µ tth ggh =.9 =.8 +.8 +.9 -.94 -.6 3 4 6 +.37 µ HIG4-9 Parameter value =.6 VBF -.34 Josh McFayden Top 7/9/

8 Josh McFayden Top 7/9/ th leptons Analysis strategy Search for single top+h production in leptonic channels Focus on the H WW* and H ττ decay modes. l SS (e ± μ ± and μ ± μ ± ) and 3l selections Several discriminating kinematic variables are combined into a single likelihood discriminant for each channel. The dominant backgrounds: Non-prompt leptons Control regions defined by looser lepton selections then used to extract extrapolation factors back to signal regions ttw Estimated purely from MC.

th leptons Likelihood discriminant CMS Preliminary 9.6 fb (8 TeV) 3 thq (Ct = ) ttw, ttz, tth WZ W ± W ± qq Ch. Mis.Id 8 6 4 CMS Preliminary 9.6 fb (8 TeV) thq (Ct = ) ttw, ttz, tth WZ W ± W ± qq Ch. Mis.Id 4 3 CMS Preliminary 9.7 fb thq (Ct = ) thw (Ct = ) diboson, WVV ttw,ttz,tth (8 TeV) CMS Preliminary 9.7 fb thq (Ct = ) thw (Ct = ) diboson, WVV ttw,ttz,tth (8 TeV) 4 3... 3 3. 4 Forward Jet η Gap 3 CMS Preliminary 9.6 fb (8 TeV) thq (Ct = ) ttw, ttz, tth WZ W ± W ± qq.... -... Lepton Charge 3 thq (Ct = ) CMS Preliminary 9.6 fb (8 TeV) ttw, ttz, tth WZ W ± W ± qq Ch. Mis.Id - - total charge 4 3 CMS Preliminary 9.7 fb thq (Ct = ) thw (Ct = ) diboson, WVV ttw,ttz,tth (8 TeV) 3 4 3 4 η(q,b) CMS Preliminary 9.7 fb thq (Ct = ) thw (Ct = ) diboson, WVV ttw,ttz,tth (8 TeV) 9. 3 3. 4 4.. 6 6. 7 (p > GeV) N jets T 3... 3 φ (l, l ) 4 6 8 #central jets 4 3 4 min ( R(l,l)) Josh McFayden Top 7/9/

th leptons Likelihood discriminant 3 thq (Ct = ) CMS Preliminary 9.6 fb (8 TeV) ttw, ttz, tth WZ W ± W ± qq Ch. Mis.Id thq (Ct = ) thq (Ct = ) thw (Ct = ) thw (Ct = ) 4 4 CMS Preliminary 9.6 fb (84 TeV) CMS Preliminary 9.6 fb (8 TeV) diboson, WVV CMS Preliminary 9.6 fb (8 diboson, TeV) WVV 6 4 ttw,ttz,tth ttw,ttz,tth e ± µ ± µ ± µ ± channel thq (Ct = ) channel thq (Ct = ) 3 lepton channel 3 3 thq (Ct = ) ttw, ttz, tth 3 ttw, ttz, tth ttw, ttz, tth WZ WZ ± ± VV, WVV W W qq ± ± W W qq 3 ttγ, ttγ* Rare SM 4 Rare SM. 4 3 Ch. Mis.Id. 3.... 3 3. 4. -... - - Forward Jet η Gap Lepton Charge - - CMS Preliminary 9.6 fb (8 TeV) CMS Preliminary 9.6 fb (8 TeV) total charge total charge 3 3 thq (Ct = ) thq (Ct = ) CMS Preliminary 9.7 fb (8 TeV) CMS Preliminary 9.7 fb (8 TeV) ttw, ttz, tth ttw, ttz, tth WZ WZ W ± W ± qq W ± W ± qq thq (Ct = ) thq (Ct = ) 4 4 thw (Ct = ) thw (Ct = ) 4 Ch. Mis.Id 3 3 diboson, WVV diboson, WVV ttw,ttz,tth ttw,ttz,tth 3...3.4..6.7.8.9...3.4..6.7.8.9...3.4..6.7.8.9 thq Likelihood thq Likelihood thq Likelihood 8 6 CMS Preliminary 9.6 fb (8 TeV) thq (Ct = ) ttw, ttz, tth WZ W ± W ± qq Ch. Mis.Id CMS Preliminary 9.7 fb (8 TeV) CMS Preliminary 9.7 fb (8 TeV). 3 3. 4 4.. 6 6. 7 (p > GeV) N jets T 3... 3 φ (l, l ) 4 6 8 #central jets 4 3 4 min ( R(l,l)) Josh McFayden Top 7/9/

th leptons Results & limits The results are compatible with the SM expectation. The dominant systematic uncertainty comes from the estimation of the non-prompt lepton backgrounds. A simultaneous fit to the likelihood discriminators is used to extract the signal cross section upper limit. Combined 9% CL upper limit assuming Ct= on σ/σsm: observed: 6.7, expected:. +. 3.4 ± 33.34 ± 8.34 63.74 ±.46 3.44 ± 6. Total Background 6.7± 8.9.3± 3.3 39.± 6. th(tt)w. ±..3 ±.4. ±. th(ww)w.8 ±.9.47 ±.48.3 ±.3 th(tt)q.9 ±.6.9 ±.9.6 ±.8 th(ww)q. ±.6 3.73 ± 3.84.73 ±.8 Total Signal 3.3±.7.± 3.98.76±.93 66 7 4 limit on σ/σ Ct= 9% C.L. CL S 3 CMS Preliminary 9.7 fb (8 TeV) pp thq t blν, H WW C t =, m = GeV H CL S Observed CL S Expected ± σ CL S exp. ± σ CL S exp. µ ± µ ± ± µ ± e 3 Leptons Combination Josh McFayden Top 7/9/

Josh McFayden Top 7/9/ ATLAS & CMS Combination Recently ATLAS & CMS published the Run combined measurements of the Higgs production and decay rates and constraints on its couplings. This includes the combined value for the tth signal strength: μ tth =.3 +.7 -.6 Significance: 4.4σ (.σ expected) Total combined signal strength: μ =.9 +. -.

3 Josh McFayden Top 7/9/ Summary and outlook First searches for the production of a Higgs boson in association with top(s) has been performed during Run These have allowed direct measurement of magnitude and sign of top Yukawa coupling, a key parameter of EWSB in SM The prospects for t[t]h measurements are good in Run-. Improvement upon on Run sensitivity should be fast. At 3 TeV the tth cross section is a factor of 4 larger than in Run. Greater precision for top Yukawa measurement. (pp H+X) [pb] pp H (NNLO+NNLL QCD + NLO EW) pp qqh (NNLO QCD + NLO EW) pp WH (NNLO QCD + NLO EW) pp ZH (NNLO QCD + NLO EW) pp bbh (NNLO and NLO QCD) pp tth (NLO QCD) = GeV MSTW8 7 8 9 3 4 s [TeV] M H LHC HIGGS XS WG 4

4 Josh McFayden Josh McFayden MC performance Top // 7/9/ Back-ups

Josh McFayden Top 7/9/ tth γγ Selection Objects: γ: ET>.3,. mγγ, η <.37 (excl. transition region),<mγγ<6 e: ET> GeV, η <.37, [E,p]Tcone/pT<%,% E T (e) μ: pt>, η <.7 [E,p]Tcone/pT<%,% pt(μ) jets: pt > GeV and η <., btagging (8TeV): 6%,7%,8% working points: Leptonic: l, bj(8%), ETmiss> GeV, Z-veto: 84<m eγ <94 GeV Hadronic: 6j bj(8%), j(3 GeV) bj(7%), 6j(3 GeV) bj(6%)

tth γγ Generators The tth signal is modelled using the PYTHIA6. The background processes ttw, ttz, tt+jets, Drell Yan+jets, W+jets, ZZ +jets, WW+jets, and WZ+jets are all generated with the MADGRAPH. The rare WWZ, WWW, tt + γ+jets, and ttww processes are generated similarly. Single top is generated with POWHEG. tth: PowHel"+Pythia8 thqb: MadGraph+Pythia8 (4-FS) WtH: MadGraph_aMC@NLO+Herwig++ (-FS) ggh and VBF: Powheg+Pythia8 VH: Pythia8 6 Josh McFayden Top 7/9/

tth γγ Yields & uncertainties 7 Josh McFayden Top 7/9/ <mγγ<3 GeV:

tth leptons Selection CMS b-tagging: medium:7% eff, % mistag, loose:8% eff, % mistag ATLAS: jets: p T > GeV and η <., b-tagging: eft 7%, % mistag p T (l)> GeV τ had p T > GeV and η <.47 lτ had : p T (l)>, GeV, [E,p T ] cone /p T :<., η(e) <.37 3l: Σq(l)=±, p T (l)> GeV (same charge l) lτ had : p T (l)>, GeV, τ had opposite charge to l s lτ had : p T (l)>, GeV, τ had opposite charge to l s 4l: Σq(l)=, p T (l)>, GeV, <m 4l < GeV, Z enriched/depleted ll=sfos 8 Josh McFayden Top 7/9/

tth leptons Yields 9 Josh McFayden Top 7/9/

tth leptons Systematic uncertainties 3 Josh McFayden Top 7/9/

3 Josh McFayden Top 7/9/ tth leptons ATLAS ttv background Validation regions for the ttv background. ttz and ttw enhanced regions to validate MC against data / GeV ATLAS 4 ttw 4 s = 8 TeV,.3 fb Rare Total unc. VV ttz VR 3 tth() ttz 3 3 s = 8 TeV,.3 fb t t W VR ATLAS Preliminary Rare 3 Charge misid tth() VV ttz ttw / Bkg 3 / Bkg 3 3 m ll [GeV] 3 Number of jets

tth leptons Other signal regions - Njets 4 ATLAS s = 8 TeV,.3 fb lτ had category ttw Total unc. tth() Rare 3 4 6 7 8 Number of jets VV ttz 8 6 4 lτhad 8 lτhad 4l 6 4 ATLAS s = 8 TeV,.3 fb lτ had category ttw Rare 3 4 6 7 8 Number of jets tt Total unc. tth() X.4 VV ttz 4 ATLAS s = 8 TeV,.3 fb 4l category ttw Total unc. tth() Rare 3 4 6 7 8 Number of jets VV ttz CMS tth, µ ± µ ± channel s = 8 TeV, L = 9. fb ± µ ± CMS tth, e channel s = 8 TeV, L = 9. fb 3 tth tth 3 tth 3 l(μμ) ttw l(eμ) ttw ttz/γ* 4l ttz/γ* ttz/γ* ZZ WZ 4 ttγ. Non Pr Others WZ Others Non Pr Others tth x tth x 3 Non Pr Ch misid. tth x. CMS tth, 4l channel s = 8 TeV, L = 9. fb 3 4 6 N(jet).... 4 6 N(jet) 4 3.. 3 3. N(jet) Josh McFayden Top 7/9/

tth leptons CMS τhad tth(.6) x 3 tt 8 6 4 CMS tth τh τ h s = 8 TeV, L = 9.3 fb Lep + τ h τ h + jets + b-tag 3 3 CMS tth τh τ h s = 8 TeV, L = 9.3 fb Lep + τ h τ h + 3 jets + b-tags Single t tt + W,Z EWK 8 6 4 Bkg. Unc. /MC Fit ±σ Fit ±σ -.8 Fit ±-.6 σ -.4 Fit ±-. σ..4.6.8 -.8 -.6 -.4 -...4.6.8 BDT output /MC -.8 -.6 -.4 -...4.6.8 BDT output 33 Josh McFayden Top 7/9/

tth leptons Generators The tth signal is modelled using the PYTHIA6. The background processes ttw, ttz, tt+jets, Drell Yan+jets, W+jets, ZZ+jets, WW+jets, and WZ+jets are all generated with the MADGRAPH. The rare WWZ, WWW, tt + γ+jets, and ttww processes are generated similarly. Single top is generated with POWHEG. 34 Josh McFayden Top 7/9/

ttv 8 TeV results 3 Josh McFayden Top 7/9/

tth leptons ℓτhad event display Event display for candidate event in the ℓτhad category. Muon Electron, pt = 8, 3 GeV Non-b-tagged jets 36 pt = GeV b-tagged jets pt = 6 GeV τ candidate pt = 4 GeV pt = 76, 6 GeV Josh McFayden Top 7/9/

37 Josh McFayden Top 7/9/ tth leptons μtth μ extraction dependant on ttw and ttz cross sections:

38 Josh McFayden Top 7/9/ th leptons Yields and uncertainties Process µµ eµ ``` W ± W ± qq 4.6 ±.68 6.3 ±.8 WZ, WW, ZZ.47 ±. 8.83 ± 3..9 ±.4 Rare SM bkg..4 ±.68.7 ±.3. ±.3 ttg. ±..4 ±.4 ttg.9 ±.3. ±.6 ttz.3 ±.4.87 ±.. ±.36 ttw ±.8 ±.4 4.8 ± 3.3 3.3 ±. tth.6 ±.34 3.4 ±.47. ±.8 Charge Mis-ID 6.96 ±.76 33.34 ± 8.34 63.74 ±.46 3.44 ± 6. Total Background 6.7± 8.9.3± 3.3 39.± 6. th(tt)w. ±..3 ±.4. ±. th(ww)w.8 ±.9.47 ±.48.3 ±.3 th(tt)q.9 ±.6.9 ±.9.6 ±.8 th(ww)q. ±.6 3.73 ± 3.84.73 ±.8 Total Signal 3.3±.7.± 3.98.76±.93 66 7 4 yields and post-fit expected backgrounds after the likelihood pre ± ± Source of uncertainty Type Exclusive Removal (%) source (%) Luminosity rate < < Pileup rate < < Lepton trigger efficiency rate < < Lepton selection efficiencies rate < < Electron energy scale shape < < Jet energy corrections shape < < b-tagging efficiencies shape < < Flavour Scheme rate Higgs branching fractions rate < < Renormalization/factorization scale rate < < Parton density functions (pdf) rate < < Irreducible background normalization rate < < µ fake-rate normalization (SS) rate 6 9 e fake-rate normalization (SS) rate µ fake-rate leptons shape (SS) shape < e fake-rate leptons shape (SS) shape < Non-prompt closure test (3`) rate 3 3 QCD control region variation for fake-rate (3`) shape < Fake-rate variation within stat. uncert. (3`) shape < Charge misidentification (SS) rate < < Stat. uncert. for non-prompt leptons (3`) shape 3 Stat. uncert. for non-prompt leptons (SS) shape 4 3 le 4: Summary of the impact of single systematic uncertainties. Deterioration of a hypot