1 / 20

W Studies at LEP2

W Studies at LEP2. SDM Elements and Polarised Cross-Sections Test of CP and CPT Invariance W Polarisation, W Polarisation vs. cos θ W WW Spin Correlations in Flight Direction WW Decay Plane Correlations. R.Ofierzynski, ETH Z ürich, on behalf of the LEP collaborations.

kenny
Download Presentation

W Studies at LEP2

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. W Studies at LEP2 • SDM Elements and Polarised Cross-Sections • Test of CP and CPT Invariance • W Polarisation, W Polarisation vs. cos θW • WW Spin Correlations in Flight Direction • WW Decay Plane Correlations R.Ofierzynski, ETH Zürich, on behalf of the LEP collaborations International Europhysics Conference on High Energy Physics 2003

  2. W Polarisations • Mass 0 – photon → helicities (–1), (+1) • Massive W boson → helicities (-1), (+1) and (0) (-1),(+1): transverse polarisation, (0): longitudinal polarisation • Standard Model: longitudinal d.o.f. from electroweak symmetry breaking mechanism • Equivalence theorem: longitudinal gauge bosons ≈ Goldstone bosons R.Ofierzynski

  3. Spin Density Matrix (D,L,O) • Theoretically: [M.Bilenky et al, Nucl.Phys.B409(1993)] e+(l’) e–(l) → W+(t2) W–(t1) → 4f (l = -l’ = ±½, t1,t2 = ±1,0) • Two-particle SDM: • Single-particle SDM: (9 elements) • diagonal elements (real) → probability to produce W- with helicity +1,0,-1 • off-diagonal elements (complex) → test of CP and CPT invariance R.Ofierzynski

  4. SDM Measurement (D,L,O) • Experimentally: divide cos θW in 8 bins • Apply projection operators on the events in bin k • : projection operator for diagonal SDM elements dependent on (cos θ*f) for non-diagonal SDM elements dependent on (cos θ*f) and Φ*f • correct for detector acceptance, resolution effects, background contamination → compare to SM prediction R.Ofierzynski

  5. SDM – Elements DELPHI preliminary measurement performed in three energy bins: 189 GeV, 192-202 GeV, 204-208 GeV SDM elements measured with W→ℓν as function of cos ΘW- R.Ofierzynski

  6. SDM – Test of CP(T) invariance L3, 189-209 GeV, W→ℓν • CPT-invariance: • CP-invariance: compatible with 0, no CP- or CPT-violation at tree level

  7. SDM – Test of CP invariance OPAL, 183-209 GeV, W→ℓν Construct CP-odd observables: consistent with 0 →TGC-parameters ≤O(10-1) — SM prediction R.Ofierzynski

  8. SDM – Polarised Cross-sections DELPHI preliminary Polarised cross-section: — SM MC prediction R.Ofierzynski

  9. SDM – Polarised Cross-sections OPAL preliminary 183-209 GeV 680pb-1, stat.+syst. uncertainty SDM elements ρ00,ρ-- measured with W→ℓν, W→qq as function of cos ΘW- Polarised cross-section — SM prediction (luminosity averaged) R.Ofierzynski

  10. W– (–1) W– (+1) W–(0) Inclusive Measurement (L3) Polar decay angle in W rest frame cos θf* W→ℓν: W→qq: Helicity fractions extracted by fit of corrected cos θ* distributions with R.Ofierzynski

  11. Inclusive W Polarisation L3, 183-209 GeV, 685pb-1, WW→e/μνqq, corrected R.Ofierzynski

  12. Longitudinal Polarisation in D,L,O • DELPHI, OPAL: integration of differential polarised cross-sections, divide by total cross-section • L3: inclusive measurement R.Ofierzynski

  13. Polarisation vs. cos ΘW- Direct measurement 183-209 GeV, W→ℓν and W→qq combined strong variations with W scattering angle, in agreement with Standard Model R.Ofierzynski

  14. WW Spin Correlations (L3) W → qq W → ℓν f–, f+, f0 (±1) depleted (±1) enriched f–, f+, f0 Relative cross-section contributions (0) difference = indicator for correlations 61.7% (±1) 89.2% (±1) (±1) |cos θ*q| R.Ofierzynski

  15. WW Spin Correlations cont. Enlarge possible effects using W scattering angle Forward bin: 0.3 < cos ΘW- < 0.9 f(–+) ≈ 63% (average 43%) Backward bin: -0.9 < cos ΘW- < -0.3 f(00) ≈ 25% (average 9%) cos ΘW- R.Ofierzynski

  16. WW Spin Correlations Results 189-209 GeV, corrected W→ℓν seen with 2.6σ, somewhat stronger than in MC R.Ofierzynski

  17. WW Spin Correlations Results 189-209 GeV, corrected W→ℓν R.Ofierzynski

  18. f f W– W+ f f Decay Plane Correlations (L3) • determine angle between decay plane normal vectors • fit with D = correlation parameter • WW→e/μνqq and WW→qqqq, 189-209 GeV [Duncan,Kane,Repko, Nucl.Phys.B272(1986)] R.Ofierzynski

  19. Decay Plane Correlations Results D = 0.000 ± 0.024 ± 0.014 D = 0.051 ± 0.033 ± 0.020 combined data: D = 0.017 ± 0.019 ± 0.011 (MC: D = 0.010 ± 0.002 ) R.Ofierzynski

  20. Conclusions • Spin Density Matrix measurement (DELPHI,L3,OPAL) Inclusive measurement (L3) • Fraction of longitudinal polarisation, variation with W scattering angle, polarised cross-sections in agreement with SM • SDM provides direct test for CP(T) invariance, no deviations from SM • expect limits on CP-violating couplings • WW spin correlations in flight direction observed with 2.6 standard deviations • WW decay plane correlations very small, in agreement with SM R.Ofierzynski

More Related