The Tevatron s Search for High Mass Higgs Bosons

Similar documents
D0 Higgs Results and Tevatron Higgs Combination

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

Searching for the Higgs at the Tevatron

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

Improvements on the Higgs searches in the high mass region at CDF

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

Higgs Searches at CMS

Inclusive top pair production at Tevatron and LHC in electron/muon final states

Higgs Boson Physics at the Tevatron

Higgs Boson Searches at ATLAS

Search for Higgs to tt at CMS

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

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

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

Search for High Mass SM Higgs at the Tevatron

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

Searches for SM H ττ at the LHC

Higgs Boson Searches in ATLAS

Standard Model Higgs Searches at the Tevatron (Low Mass : M H ~140 GeV/c 2 )

Highlights of top quark measurements in hadronic final states at ATLAS

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

ATLAS-CONF October 15, 2010

Tevatron Physics Prospects. Paul Grannis, for the CDF and DØ collaborations ICFA Seminar, Oct

Higgs search in WW * and ZZ *

Status of ATLAS Higgs Search

PoS(EPS-HEP2011)250. Search for Higgs to WW (lνlν, lνqq) with the ATLAS Detector. Jonas Strandberg

Search for the Higgs Boson In HWW and HZZ final states with CMS detector. Dmytro Kovalskyi (UCSB)

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

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

Combined Higgs Results

Combination of Higgs boson searches at ATLAS

Single top quark production at CDF

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

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

PoS(DIS 2010)190. Diboson production at CMS

Search for Higgs in H WW lνlν

Top production at the Tevatron

PoS(ICHEP 2010)544. Higgs searches at the Tevatron. Ben Kilminster Fermilab bjk AT fnal.gov

Search for SUSY at CMS in lepton or photon final states. PANIC 2011 K. Theofilatos (on behalf of CMS)

Searches for Standard Model Higgs Boson at the D Detector at the Tevatron. Alexander Khanov Oklahoma State University SUSY 06

Single-Top at the Tevatron

Combined Higgs Searches at DZero

Recent ATLAS measurements in Higgs to diboson channels

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

Top production measurements using the ATLAS detector at the LHC

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

Discovery potential of the SM Higgs with ATLAS

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

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

Measurements of the Higgs Boson at the LHC and Tevatron

Summer plans and prospects on Higgs searches at DZero Yuji Enari D0 France meeting 1

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

Pedro Teixeira-Dias. Higgs Overview

Recent Results on Top Physics at CMS

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

Search for Charginos and Neutralinos with the DØ Detector

ATLAS NOTE ATLAS-CONF th March 2015

Yoshikazu NAGAI (CPPM, Aix Marseille Université)

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

WZ di-boson production at CMS

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

Recent Results from the Tevatron

Search for the High-Mass Standard Model Higgs Boson with the ATLAS Detector

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

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

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

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

Search for Dark Matter in the mono-x* final states with ATLAS

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

Title Text. ATLAS Higgs Boson Discovery Potential

ATLAS Discovery Potential of the Standard Model Higgs Boson

Searches for Physics Beyond the Standard Model with the ATLAS Detector

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

} Very nice new results on limits

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

Search for Resonant Slepton Production with DØ

Top and Electroweak Physics at. the Tevatron

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

Ernest Aguiló. York University

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

La ricerca dell Higgs Standard Model a CDF

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

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

Beyond the Standard Model Higgs boson searches using the ATLAS etector

Top Quark Physics at the LHC

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

Top physics at CDF. Journal of Physics: Conference Series. Related content

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

CMS Higgs Results Adi Bornheim Caltech

Higgs and Z τ + τ in CMS

Evidence for Single Top Quark Production. Reinhard Schwienhorst

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

Statistical Tools in Collider Experiments. Multivariate analysis in high energy physics

CMS Searches for New Physics

Single Top At Hadron Colliders

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

2016 SM H ττ Analysis 26th September 2016

Taller de Altas Energías Michael Holzbock September 7, LMU Munich

BSM Higgs Searches at ATLAS

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

Transcription:

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 Higgs Searches Moriond EW March 2011 1 / 27

High mass Higgs searches at the Tevatron Higgs production cross sections for p p collisions at s = 1.96 TeV Gluon fusion (ggh) σ 0.2 1 pb Associated production (VH) σ 0.01 0.3 pb Vector Boson Fusion (qqh) σ 0.01 0.1 pb Precision ewk data yields 114 <M H < 186 GeV @95 C.L High Mass definition: Searches most sensitive for M H 135 GeV Main Decay mode is WW K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 2 / 27

H WW Final States Use of all feasible final states Hadron collider environment requires at least one leptonic W decay Dilepton (e, µ) - BR 6% Most sensitive final state Lowest Background Rate W Branching Fractions Lepton (e, µ)+τ h - BR 4% Consider hadronic τ decays (τ h ) Provides additional sensitivity Larger Background Rate e, µ+hadrons - BR 30% Larger BR gives 5 more signal compared to Dilepton Large Background Rate K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 3 / 27

High Masss Higgs Search Strategy Very low S/B makes a cut based analysis impossible (0.1 1.)% for m H = 165 GeV @ final selection stage Not a counting experiment Employ use of Multivariate techniques (MVA) to extract the signal Maximise power of discriminating variables Input parameters: Kinematic and Event topology variables MVA outputs used as inputs for limit setting (Neural Networks, Decision Trees) Technique validated measuring SM processes Create as many sub-channels as possible Optimise our Signal/Background discriminants for different mixes of signal and background contributions K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 4 / 27

Status in Summer 20 Combining low mass and high mass Using 5.6-6.1 fb 1 of analyzed data DØ almost achieved observed exclusion at M H = 165 GeV CDF achieved excpected exclusion at M H = 165 GeV Work even harder to improve sensitivity! K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 5 / 27

What is new in March 2011 CDF and DØ updated High Mass program using up to 7.1 fb 1 and 8.2 fb 1 respectively Channel CDF DØ H WW l νl + ν l = e, µ, 0/1/2+ jet Add data New l = e, µ, 1 jet low M ll Add data - l = τ h, µ(e) Add data New l = τ h, µ(e), 2+ jet - New (4.3 fb 1 ) H WW lνqq l = e, µ, 2+ jet - (5.4 fb 1 ) VH VWW SS Dilepton Add data (5.4 fb 1 ) Trileptons Add data - K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 6 / 27

H WW l νl + ν Event Selection 2 Opposite Sign high p T isolated leptons distinguishes from multijet and W+jets Missing Energy from neutrinos distinguishes from Z/γ Final state topology due to spin 0 Higgs distinguishes from WW Small opening angle between leptons in Higgs decays K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 7 / 27

H WW l νl + ν (l = e, µ) Splitting into sub-channels I Lepton Flavour DØ: eµ,ee,µµ CDF: Lepton flavour or quality Separation gives high and low S/B regions Entries 5 4 3 2 1 DØ Preliminary 1 L = 8.1 fb ee + MET data Z+jets Diboson W+jets Multijet ttbar Different efficiency, kinematics and resolution 1 0 20 40 60 80 0 120 140 160 180 200 M ee (GeV) Signal (M = 165 GeV) H Entries 4 data 1 3 DØ Preliminary L = 8.1 fb eµ + MET Z+jets Entries 5 4 DØ Preliminary 1 L = 8.1 fb µµ + MET data Z+jets Diboson 3 Diboson 2 W+jets 2 W+jets Multijet Multijet 1 0 0.5 1 1.5 2 2.5 3 φ eµ ttbar Signal (M = 165 GeV) H 1 1 0 20 40 60 80 0 120 140 160 180 200 M µµ (GeV) ttbar Signal (M = 165 GeV) H K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 8 / 27

H WW l νl + ν (l = e, µ) Splitting into sub-channels II Jet Multiplicity: 0jet, 1jet, 2jets Optimise on different signal/background compositions 0jet: WW 1jet: Z/γ 2jet: t t K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 9 / 27

e H WW l νl + ν (l = e, µ) Final Event Selection Reduce large Z/γ using E miss T DØ: Train DT against Z/γ for ee,µµ Each jet bin and mass hypothesis E miss T related variables as inputs Select events in high DT region CDF: Select events with high E miss T 0 signal evts at Final Selection (CDF+DØ) @M H = 165 GeV Jet bin splitting and Z/γ DT improves DØ s expected sensitivity 30% @M H =130GeV 15% @M H =165GeV Entries Entries 5 4 3 2 1 1 DØ Preliminary 1 L = 8.1 fb ee + MET 2 0 20 40 60 80 0 120 140 160 180 200 5 4 3 2 1 1 H WW µµ, 0 jets E T (GeV) Preliminary 1 0.8 0.6 0.4 0.2 0 0.2 0.4 0.6 0.8 1 RF_Dy 0jets data Z+jets Diboson W+jets Multijet ttbar 6 data DØ Preliminary µµ+met+2jets M H =165 GeV Signal (M = 165 GeV) H KS Prob=8.993000e 01 Z+jets Diboson W+jets Multijet ttbar Sig Tot 1 Sig gghww Sig WH Sig ZH 1 1 Sig VbfH 1 Sig gghzz 1 1 K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 / 27

H WW l νl + ν (l = e, µ) Extract Signal Train MVA using Final Selection events in each jet bin and mass Input discriminating variables: Likelihood ratio of Matrix Element calculation (0jet CDF) Topological+kinematic combos Transverse mass of vector sum of lepton p and E miss T Use b-tagging information as input variable or veto in 1 or 2jet bin against t t K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 11 / 27

H WW l νl + ν (l = e, µ) MVA distributions CDF: NN DØ: DT Events 2 H WW eµ, 0 jets DØ Preliminary eµ+met+0jets M H =165 GeV Preliminary data Z+jets Events 3 data 2 H WW ee, 1 jets Preliminary DØ Preliminary ee+met+1jets M H =165 GeV Z+jets Diboson Diboson W+jets W+jets Multijet 1 Multijet 1 ttbar ttbar 1 m H =165 GeV 1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Final Discriminant Sig Tot 2 1 0.8 0.6 0.4 0.2 0 0.2 0.4 0.6 0.8 1 Final Discriminant Tot. Sig K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 12 / 27

H WW l νl + ν (l 1 = τ h l 2 = µ,e) Including τ leptons decaying to hadrons. New channels for DØ! CDF updated e + τ h and µ + τ h as well µ and hadronically decaying τ (τ h ) + 1jet 3 subchannels based on τ h track/calo structure MVA based on NN µτ h and eτ h + 2jet For M H < 135 sensitive to H ττ final state K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 13 / 27

H WW lνq q (l = e, µ) Including hadronic W decays 1 lepton 2jets+E miss T 52 expected signal events @M H =160 GeV! Main background W+jets Reconstruct p z of neutrino using W mass constraint Possible to extract Higgs mass for M H >160 GeV K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 14 / 27

VH VWW (V=W or Z) Multi-lepton and jet final states from W/Z decays Suppress SM backgrounds Same Sign Dilepton + E miss T WH WWW Lepton charge measurement important Trilepton OS same flavour pair in/out Z mass window ZH ZWW/WH WWW K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 15 / 27

Systematic Uncertainties Events/0.13 Affecting Normalization or Shape of signal and background in the final discriminant Correlated luminosity (Total:6% Correlated:4%) and x-section between CDF and DØ Lepton ID 2 4%, Jet 3 25%(process dependent) 50 40 30 20 Tevatron Run II Preliminary L 8.2 fb -1 Data-Background SM Higgs Signal ±1 s.d. on Background 0 - -20-30 -40 March 7, 2011 m H =165 GeV -50-1.8-1.6-1.4-1.2-1 -0.8-0.6-0.4-0.2 0 log (s/b) σ NNLO+NNLL ggh scale variation 7 33% jet bin dependent JHEP 0908, 099 (2009), Phys Rev D 81, 074023 (20) σ NNLO+NNLL ggh PDF uncertainty 8 30% jet bin dependent Treatment recommended by PDF4LHC group Shape systematic for resummation scale by varying NNLO+NNLL p H T spectrum Expected signal lies above background uncertainty! K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 16 / 27

Limits No significant excess of signal like events is observed MVA outputs used to set exclusion limits at 95% C.L DØ: Single Experiment Exclusion!! 163<M H <168 @95% C.L (160<M H < 168 expected) CDF: Single Experiment Exclusion!! 158<M H <168 @95% C.L (160<M H < 167 expected) K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 17 / 27

Conclusions and Outlook Presented an overview of the latest Tevatron High mass Higgs searches A great milestone achieved by both experiments reaching exclusion sensitivity individually Explore all available avenues Large Data Samples All feasible final states considered All feasible channel splittings considered Sophisticated signal/background discriminants Still room for improvement fb 1 by the end of RunII Improvements in object IDs Additional channels such as H ZZ And now for the Combined Results! (see Bo s talk coming soon) Many thanks to CDF and DØ collaborators K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 18 / 27

Backup K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 19 / 27

Expected limits per channel Exp Limit x SM @165 Channel CDF DØ H WW l νl + ν l = e, µ, 0/1/2+ jet 0.93 (incl. low M ll,ss dilep,trilep) 0.97 l = τ h, µ(e) 13.1 7.5 (µτ h ) l = τ h, µ(e), 2+ jet - 12.3 H WW lνqq l = e, µ, 2+ jet - 5.1 VH VWW SS Dilepton - 7.0 K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 20 / 27

Matrix Element Discriminant K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 21 / 27

MVA cross check K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 22 / 27

Responses I K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 23 / 27

Responses II K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 24 / 27

Responses III K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 25 / 27

Responses IV K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 26 / 27

Responses V K.A. Petridis (University of Manchester) Tevatron High Mass Higgs Searches Moriond EW March 2011 27 / 27