D. PALLIN Clermont University On behalf of the ATLAS collaboration October 2, 2012 LHC days in SPLIT BOOSTed Physics at ATLAS.

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D. PALLIN Clermont University On behalf of the ATLAS collaboration October 2, 2012 LHC days in SPLIT BOOSTed Physics at ATLAS

Motivation With increasing c.m. energies, particles tends to be more boosted, and their decay products more collimated. heavy particles produce naturally boosted objects as single massive jet Standard reconstruction of the decays products inefficient With the increasing luminosity, the number of observed boosted particle become significant in present LHC data. 2 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/ fat jet3 resolved jets

Motivation With increasing c.m. energies, particles tends to be more boosted, and their decay products more collimated. heavy particles produce naturally boosted objects as single massive jet Standard reconstruction of the decays products inefficient With the increasing luminosity, the number of observed boosted particle become significant in present LHC data To fully exploit potential signatures (at high mass) from new physics at LHC novel reconstruction techniques to handle highly boosted objects Simple Fat jet reconstruction or Jet substructure techniques to identify the hadronic decays of boosted particles. application to reconstruction of W & top hadronic decays 3 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012

BOOSTED Physics LHC explores the TeV scale :Hunting massive particles Many studies dedicated to fat jets/ using jet substructure technique in ATLAS Focusing on some recent results Heavy ttbar resonances (boosted tops) Many models of new physics BSM predict resonances in the TeV mass range that decay primarily into ttbar quark pairs 4 th generation b’  Wt,t’  Wb (boosted W) Natural extension to the SM. Generic search for heavy up/down quarks Other ongoing studies RPV gluino decay to three overlapping jets (boosted jet triplet) … 4 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012

A simple approach b’  Wt b’b’  Wt Wt  l +8jets, single lepton trigger signature :lepton+MET+≥6 jets Boosted W Approach : Semi-Boosted Ws look at jet pairs with small opening angle and m jj ~mW up to 80% selection efficiency for high pT W 5 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 [arXiv: ] Main syst. : JES, ISR/FSR M b’ > 480 BR(b’  Wt)=1 (non boosted analysis M b’ > 450 GeV )

A simple approach t’  Wb t’t’  Wb Wb  l +4jets, single lepton trigger signature :lepton+MET+≥3jets; ≥ 1b-tag jet define as the 2 b-jets, the 2 jet with higest btag Prob Boosted W Approach : exploit kinematics :Large  R(Wb) small  R(jj) W Select candidates (≥1 fat jet+3 ≥ jets) or (≥4 jets+ ≥ 1 resolved W Use kin to educe BKG:  R(Wb) >1.4 &  R(lb)>1.4 Choose W1b1W2b2 combination minimizing MW 1 b 1 – MW 2 b 2 6 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 [NEW] M t’ > 656 BR(t’  Wb)=1

A sophisticated approach tt resonances X  tt  WbWb Two specific models that predict resonances with narrow and broad decay widths are used as benchmarks: Leptophobic topcolour Z’, spin 1 with  /m = 1.2% Eur. Phys. J. C72 (2012) 2072 Kaluza-Klein (KK) gluons from RS models, spin 1 with  /m = 15.3% Phys.Rev. D76 (2007) ; JHEP 0709 (2007) 074 Reconstruction with standard jets and by exploiting jet substructure Channels : lepton+jets, all-jets. 7 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 channelResolved analysisBoosted analysis All-jets 4,7fb-1 ATL-CONF Lepton( e,µ)+jets 4,7fb-1 ATL-CONF

A sophisticated approach tt resonances X  tt  WbWb ? a tt candidate (m=2.5 TeV) with a highly boosted hadronic top Jets reconstructed with R = 0.4 in green circles, with R = 1.0 in red circles 8 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012

A sophisticated approach tt resonances Boosted Techniques Investigation of the substructure Soft radiation, Underlying event & pile-up in the fat jet dilute substructure “grooming” allows to extract substructure. Three main techniques : pruning [Ellis, Vermilion, Walsh; 2009] filtering [Butterworth, Davison, Rubin, Salam; 2008] Trimming [Krohn, Thaler, Wang; 2010] ATLAS studies to gain confidence in subjet/boosted techniques [arXiv: ] jet mass and subjet variables [arXiv: ] properties of boosted jets ATLAS HEPToptagger for reconstruction and tagging specfic to Top quark [atl-conf ] [atl-conf ] using filtering like approach. 9 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 MC predictions are found broadly in agreement with data

A sophisticated approach tt resonances HEPTopTagger HEPToptagger for reconstruction and tagging specfic to Top quark Filtering : Iterative clustering : seeks to isolate concentrations of energy within a jet by identifying relatively symmetric subjets, each with a significantly smaller mass than that of their sum Start from the two subjets of the fat jet from the last stage of clustering of C/A jet algorithm Mass-drop: Decompose jets until m ji at least 3 subjets Filtering :re-cluster with Rfilt = min[0:3;  Rj1; j2/2 ] build exactly 3 subjets from the selected constituents with mass constraints  Rejection of UE/pile-up deposits  Sub-jets reconstruction  Reclustering to 3 sub-jets with mass constraints 10 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012

A sophisticated approach tt resonances HEPTopTagger HEPTopTagger performance [atl-conf ] using tt  WbWb  l +4jets Single muon trigger, ≥4 jets (AKT4), MET jets with R=1.5 before HEPTopTagger after HEPTopTagger 11 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012

A sophisticated approach tt resonances All-jet Channel tt  WbWb  6 jets High pT jets trigger, mini-isolation lepton veto, ≥2 fat jets(C/A,R=1.5) with pT>200GeV, ≥2 b-tag jets(AKT4) tt reconstruction 2 jets HEPTOPtagger (Mt not impacted by PU) Build Di-top invariant mass SM top pairs normalisation from a fit in Control region QCD multijet from control regions 12 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 No excess observed

A sophisticated approach tt resonances All-jet Channel Limits limits for Z’ KK gluon 13 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 Exclusion 0.7 TeV <m Z’ <1.3TeV 0.7 TeV <m gKK <1.5TeV

A sophisticated approach tt resonances Lepton+jet Channel tt  WbWb  l +4jets resolved: Single lepton trigger, ≥4 jets (AKT4), MET, ≥1 b-tag resolved semi-boosted(W boosted) : Single lepton trigger, ≥3 jets (AKT4) with 1 jet m>60GeV, MET, ≥1 b-tag boosted: fat jet (AKT10) trigger, 1 lepton (mini-isolation), 1 leptonic jet (AKT4), fat jet p T >350 GeV, m>100Gev,  d 12 >40GeV, ≥1 b-tag tt reconstruction neutrino momentum reconstruction using MET and M W constraint resolved: use combination with lowest  2 using M W and M top constraints boosted: using lepton+neutrino + nearest from lepton AKT4 +AKT10 jet 14 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 Resolved : low tt mass range Resolved semi-boosted: intermediate mass range Boosted : high mass range No excess observed

A sophisticated approach tt resonances Lepton+jet Channel Limits Use boosted reconstruction if event select by resolved & boosted Some events at high mass from resolved reconstruction limits for Z’ resolved boosted 15 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012 Complementary approach, better sensitivity at low mass for resolved, at high mas for boosted Combined limit of boosted+resolved Exclusion 0.5 TeV <m Z’ <1.7TeV 0.7 TeV <m gKK <1.9TeV

Summary Jet substructure techniques to identify the hadronic decays of boosted heavy particles demonstrated that they are key feature for massive particle search at LHC. With increasing c.m. energy and luminosity, Boosted techniques will gain in importance in the future No evidence for new physics in boosted physics found yet, but reached mass range increased significantly thanks to boosted techniques 16 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012

A sophisticated approach tt resonances HEPTopTagger Investigation of the substructure HEPToptagger for reconstruction and tagging specfic to Top quark Soft radiation, Underlying event & pile-up in the fat jet dilute substructure “grooming” allows to extract substructure. Three main techniques : pruning [Ellis, Vermilion, Walsh; 2009] filtering [Butterworth, Davison, Rubin, Salam; 2008] Trimming [Krohn, Thaler, Wang; 2010] Pruning : discard soft & wide angle particles. 17 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012

A sophisticated approach tt resonances HEPTopTagger Investigation of the substructure HEPToptagger for reconstruction and tagging specfic to Top quark Soft radiation, Underlying event & pile-up in the fat jet dilute substructure “grooming” allows to extract substructure. Three main techniques : pruning [Ellis, Vermilion, Walsh; 2009] filtering [Butterworth, Davison, Rubin, Salam; 2008] Trimming [Krohn, Thaler, Wang; 2010] Trimming :. 18 LHC days in Split / BOOSTed Physics at ATLAS D. Pallin 2/10/2012