WW Fusion in Higgsless Models at the LHC

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WW Fusion in Higgsless Models at the LHC Rahul Malhotra University of Hawaii at

WW Fusion in Higgsless Models at the LHC Rahul Malhotra University of Hawaii at Manoa PHENO 2006

Higgsless Models • Theories contain tower of heavy Te. V-scale vector bosons - Vi±,

Higgsless Models • Theories contain tower of heavy Te. V-scale vector bosons - Vi±, Vi 0 • O(E 4) and O(E 2) terms in the WW, WZ scattering amplitudes are cancelled by exchange of these particles, without invoking a Higgs boson • In 5 D theories symmetry-breaking is achieved via boundary conditions on an interval • Unitarity violation postponed to Λ ~ 5 – 10 Te. V [ Cacciapaglia, Csaki, Grojean, Pilo, Murayama, Terning hep-ph/0305237, 0308038, 0401160, 0409126 ]

← Resonance [ Chivukula, Dicus, He, Nandi hep-ph/0111016, 0302263, 0402222; Csaki hep-ph/0510275 ] SUM

← Resonance [ Chivukula, Dicus, He, Nandi hep-ph/0111016, 0302263, 0402222; Csaki hep-ph/0510275 ] SUM RULES :

WZ → V 1± → WZ • The sum rules were found saturated by

WZ → V 1± → WZ • The sum rules were found saturated by just one resonance V 1± : • SM fermions can be decoupled from excited KK modes* • “Gold - plated” channel: 2 forward jets + 3 l + missing ET • M upto 1 Te. V covered by 60 fb-1 of luminosity [ Birkedal, Matchev, Perelstein hep-ph/0412278 * Cacciapaglia et al hep-ph/0409126 ]

WW → V 10 → WW LHC Signal: 2 forward jets + final state

WW → V 10 → WW LHC Signal: 2 forward jets + final state W Decays: 1. ll 2. l jj • Cleaner Signal • Cannot reconstruct mass • More background sources • Can reconstruct mass

Backgrounds for eμ - channel Top production dominates background even after cuts • •

Backgrounds for eμ - channel Top production dominates background even after cuts • • tt + jets EW WWjj in SM QCD WWjj production + jets ~ 50 -70% ~ 20 -40% ~ 5 -10% < 5%

Controlling Backgrounds: • 2 separated forward jets: | 1 - 2| > 4. 4

Controlling Backgrounds: • 2 separated forward jets: | 1 - 2| > 4. 4 • b, Minijet Veto in central region for ET > 20 Ge. V. • Require forward jets MJJ > 700 Ge. V • Reconstruct (gentle) resonance in ETmax (e, μ) > 85 Ge. V for MV = 500 Ge. V ↓ > 140 Ge. V for MV = 1 Te. V • Real reconstruction

More on central jet veto • Adopt similar methodology to that used for heavy

More on central jet veto • Adopt similar methodology to that used for heavy higgs H → WW searches • For example for tt + jets: - Calculate tt, tt + 1 j, tt + 2 j - Use higher order calculation to estimate central jet activity - Veto central b jets with ET > 20 Ge. V [ Rainwater, Zeppenfeld hep-ph/9906218 ]

LHC Cross-sections (fb), MV = 725 Ge. V CUTS V 10 jj WWjj (EW)

LHC Cross-sections (fb), MV = 725 Ge. V CUTS V 10 jj WWjj (EW) WWjj (QCD) tt + jets 2 forward jets + ET(l) > 20 Ge. V, | (l)| < 2. 5 0. 668 2. 84 4. 71 1036 MJJ > 700 Ge. V 0. 602 2. 64 2. 45 414 Veto central b jets / minijets 0. 522 2. 06 0. 637 6. 54 ETmax(e, μ) > 110 Ge. V 0. 418 0. 803 0. 113 1. 11

RESULTS MV Discovery Range (Ge. V) 30 fb-1100 fb-1 300 fb-1 5 366 535

RESULTS MV Discovery Range (Ge. V) 30 fb-1100 fb-1 300 fb-1 5 366 535 723 4 420 610 816 3 503 717 960 • Challenging • Can be improved by - including ee, μμ + neutrinos channel - more refined cuts • Aim to extend 5 to 1 Te. V at 300 fb-1