Presentation is loading. Please wait.

Presentation is loading. Please wait.

W - TGCs at a γγ – collider at TESLA

Similar presentations


Presentation on theme: "W - TGCs at a γγ – collider at TESLA"— Presentation transcript:

1 W - TGCs at a γγ – collider at TESLA
K.Mönig, J.Sekaric DESY-Zeuthen ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

2 Two couplings, κγ in dim-4 and λγ in dim-6 operators
Introduction Dominating diagram for γγ  W+W- TGC Two couplings, κγ in dim-4 and λγ in dim-6 operators Deviations from SM TGC values  test of EW theory, probe of some possible extensions  new physics beyond the SM q Ambiguities : (cosθ1,2,φ1,2) ↔ (-cosθ1,2,φ1,2+π) WBACKWARD y 1 x 2 x 1 z 2 z y WFORWARD q ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

3 Denner, Dittmaier, Schuster, hep-ph/9503442
ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

4 Denner, Dittmaier, Schuster, hep-ph/9503442
ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

5 Total Cross-Section - Whizard
ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

6 Deviation effects of WLL’s in presence of anomalous coupling
Differential Cross-Section Deviation effects of WLL’s in presence of anomalous coupling ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

7 Deviation effects of WLL’s in presence of anomalous coupling
Differential Cross-Section Deviation effects of WLL’s in presence of anomalous coupling ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

8 Analysis Signal (γγ→WW) sample for JZ=0(±±),2(± ) (WHIZARD – W. Kilian, 100% polarized photon beams, fixed beam energy) σhad(0)=35pb; σhad(2)=31pb Response of a detector simulated with SIMDET V4 Ws are reconstructed from hadronic final states MW=(60-100) GeV; θnenflo>7º; NENFLO>10; NCT>5; pile-up (no track rejection) 1.8 ev/BX Estimated errors of measurement of  and  parameters, obtained by binned Likelihood fit ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

9 WFORWARD WFORWARD WBACKWARD
MW1 [GeV] WFORWARD WBACKWARD ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

10 ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

11 Monte Carlo Fit Each event described with 5 kinematical variables (sensitive to TGC) : - W production angle, cosθ of forward W-boson - W polar decay angles, cosθ1,2 (sensitive to the different W helicity states) of higher energetic jet azimuthal decay angles, 1,2 (sensitive to the interference between different W helicity states) of higher energetic jet Matrix element calculations (WHIZARD-O’Mega)  weights to reweight SM events (Δκγ=0, Δλγ=0) as functions of anomalous TGC by Weight/event: R(,) = 1 + A· + B·()2 + C· + D·()2 + E ·  ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

12 ND=NSM- data sample (SM), NMC- Monte Carlo sample [NSM·R(,)], L – error on luminosity measurement ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

13 Likelihood (normalized) DETECTOR LEVEL MW1,2=(60 – 100) GeV
2 Parameter Fit Results – JZ=0 JZ=0 3D/5D (φ=0-2π) ECM = 400 GeV, L = 110 fb-1 , FBE Likelihood (normalized) DETECTOR LEVEL MW1,2=(60 – 100) GeV L 1% 0.1% accurate  ·10-4/10-4 26.0/14.4 6.2/5.4 3.8/2.6  ·10-4/10-4 14.4/3.0 13.7/3.0  ·10-4 +pileup 15.4 5.4 2.6  ·10-4 +pileup 3.8 3D  5D decreases the error in  ; in  significantly ! Pile-up distorts the φ-distribution  increase of error in  for ~20%  dependences on normalization ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

14 Likelihood (normalized) DETECTOR LEVEL MW1,2=(60 – 100) GeV
2 Parameter Fit Results – JZ=2 JZ=2 3D/5D (φ=0-2π) ECM = 400 GeV, L = 110 fb-1 , FBE Likelihood (normalized) DETECTOR LEVEL MW1,2=(60 – 100) GeV L 1% 0.1% accurate  ·10-4/10-4 29.0/19.9 6.2/6.2 3.9/3.8  ·10-4/10-4 1.8/1.5 1.6/1.5  ·10-4 +pileup 23.2 6.3 3.9  ·10-4 +pileup 2.0 3D  5D no influences in the error estimations Pile-up distorts the φ-distribution  increase of error in  for ~25%  dependences on normalization ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

15 Conclusions JZ =0,2 are sensitive to the anomalous couplings  to the possible scenarios of EWSB φ distribution important for JZ=0 Pile­up influences on λγ measurement (~25%) Promising channel for κγ - λγ measurements Δκγ, Δλγ ~ 10-4 FUTURE to include the possible backgrounds, variable beam energy rejection of bad tracks from pileup ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen

16 ANALYTIC FORMULA γγ  WW
Backup Dominated WTT fraction σWHIZARD scaled to the σFORMULA WHIZARD γγ  WW ANALYTIC FORMULA γγ  WW ECFA, Sept. 04, UK Sekaric Jadranka DESY-Zeuthen


Download ppt "W - TGCs at a γγ – collider at TESLA"

Similar presentations


Ads by Google