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Four-fermion production near the W-pair production threshold Giulia Zanderighi, Theory Division, CERN ILC Physics in Florence September 12-14 2007 International Linear Collider we all believe that no matter what will be discovered (or not)


  1. Four-fermion production near the W-pair production threshold Giulia Zanderighi, Theory Division, CERN ILC Physics in Florence September 12-14 2007

  2. International Linear Collider we all believe that no matter what will be discovered (or not) at the LHC, the ILC will provide complementary information Giulia Zanderighi − Four fermion production near the W-pair production threshold 2 /22

  3. International Linear Collider we all believe that no matter what will be discovered (or not) at the LHC, the ILC will provide complementary information given the high energy involved, the ILC can be a discovery machine, but thanks to the very clean e+e- environment the ILC will be mainly a precision machine Giulia Zanderighi − Four fermion production near the W-pair production threshold 2 /22

  4. International Linear Collider we all believe that no matter what will be discovered (or not) at the LHC, the ILC will provide complementary information given the high energy involved, the ILC can be a discovery machine, but thanks to the very clean e+e- environment the ILC will be mainly a precision machine From the high precision of the ILC we expect to ‣ identify the nature of new physics (discovered at the LHC?) by doing direct and indirect measurements of particle properties ‣ constrain new physics and model parameters (e.g. heavy masses, couplings) Giulia Zanderighi − Four fermion production near the W-pair production threshold 2 /22

  5. Precision measurements at the ILC ‣ Higgs: mass, branching ratios, width, CP , spin, couplings, [specifically top-Yukawa, Higgs self-coupling] Giulia Zanderighi − Four fermion production near the W-pair production threshold 3 /22

  6. Precision measurements at the ILC ‣ Higgs: mass, branching ratios, width, CP , spin, couplings, [specifically top-Yukawa, Higgs self-coupling] ‣ anomalous couplings ‣ electroweak parameters M Z , Γ Z , M W , Γ W , m t , Γ t , sin 2 θ W, e ff , R b , R c , R l , σ had (e.g. ) 0 ‣ QCD coupling and evolution (new color degrees of freedom?) ‣ If (SUSY) ⇒ plethora of SUSY masses and parameters ‣ If (ED) ⇒ measure M, , KK-powers δ ‣ If (XXX) ⇒ measure YYY Giulia Zanderighi − Four fermion production near the W-pair production threshold 3 /22

  7. Precision measurements at the ILC This talk M W Giulia Zanderighi − Four fermion production near the W-pair production threshold 3 /22

  8. W mass is a key observable in the search of virtual-particle M W exchange through electroweak precision measurements ⇒ can constrain by precisely t M H H measuring and M W m t ∆ M W ∝ m 2 ∆ M W ∝ ln M H t 80.5 High Q 2 except m W / Γ W experimental errors 68% CL: LEP1 and SLD 80.70 m t 2 ~ / m t 1 ~ > 2.5 ~ ,b 2 ~ ,b 1 68 % CL LEP2/Tevatron (today) LEP2 and Tevatron (prel.) 80.5 [LEPEWWG] Tevatron/LHC [LEPEWWG] Y 68 % CL S U S 80.60 h t ILC/GigaZ g l i m W [ GeV ] m W [ GeV ] [hep-ph/0611371] M W [GeV] MSSM − ) m W (LEP2 prel., pp 80.50 80.4 80.4 heavy SUSY 80.40 M H = 114 GeV 80.30 SM 80.3 SM MSSM M H = 400 GeV ∆α m H [ GeV ] both models Excluded Heinemeyer, Hollik, Stöckinger, 114 300 1000 80.3 80.20 Weber, Weiglein ’06 2 3 160 165 170 175 180 185 10 10 10 150 175 200 m t [GeV] m H [ GeV ] m t [ GeV ] Giulia Zanderighi − Four fermion production near the W-pair production threshold 4 /22

  9. W mass determination current value: = (80.403 0.029) GeV determined from ± M W combination of continuum W-pair production at LEPII and single-W at the Tevatron Giulia Zanderighi − Four fermion production near the W-pair production threshold 5 /22

  10. W mass determination current value: = (80.403 0.029) GeV determined from ± M W combination of continuum W-pair production at LEPII and single-W at the Tevatron single-W production at the LHC: expected to reduce the error by a factor 2 Giulia Zanderighi − Four fermion production near the W-pair production threshold 5 /22

  11. W mass determination current value: = (80.403 0.029) GeV determined from ± M W combination of continuum W-pair production at LEPII and single-W at the Tevatron single-W production at the LHC: expected to reduce the error by a factor 2 two techniques at the ILC: - kinematic fitting of WW production at GeV √ s = 500 ⇒ reach 5 MeV error with (several years) L = 1000 fb − 1 - threshold scan: exploit rapid variation of at threshold σ ⇒ error of 5 MeV with (just one year) L = 100 fb − 1 Giulia Zanderighi − Four fermion production near the W-pair production threshold 5 /22

  12. Some history of WW (before ’05) NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

  13. Some history of WW (before ’05) lowest order amplitudes for an onshell W-pair [Alles et al. ’77, Gaemers&Gounaris. ’79] NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

  14. Some history of WW (before ’05) lowest order amplitudes for an onshell W-pair [Alles et al. ’77, Gaemers&Gounaris. ’79] electroweak correction to onshell W-pair [Lemione&Veltman ’80, Philippe ’82, Fleischer et al. ’89, Boehm ’88] NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

  15. Some history of WW (before ’05) lowest order amplitudes for an onshell W-pair [Alles et al. ’77, Gaemers&Gounaris. ’79] electroweak correction to onshell W-pair [Lemione&Veltman ’80, Philippe ’82, Fleischer et al. ’89, Boehm ’88] electroweak correction to onshell W decay [Bardeen et al. ’86, Jegerlehner ’88, Denner&Sack et al. ‘90] NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

  16. Some history of WW (before ’05) lowest order amplitudes for an onshell W-pair [Alles et al. ’77, Gaemers&Gounaris. ’79] electroweak correction to onshell W-pair [Lemione&Veltman ’80, Philippe ’82, Fleischer et al. ’89, Boehm ’88] electroweak correction to onshell W decay [Bardeen et al. ’86, Jegerlehner ’88, Denner&Sack et al. ‘90] inclusion of hard photon radiation [Beenakker et al. ’91, Tanaka et al. ’91, Kolodziej et al. ’91, Feischer et al. ’93] NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

  17. Some history of WW (before ’05) Frontier of higher order lowest order amplitudes for an onshell W-pair calculations at the time [Alles et al. ’77, Gaemers&Gounaris. ’79] electroweak correction to onshell W-pair [Lemione&Veltman ’80, Philippe ’82, Fleischer et al. ’89, Boehm ’88] electroweak correction to onshell W decay [Bardeen et al. ’86, Jegerlehner ’88, Denner&Sack et al. ‘90] inclusion of hard photon radiation [Beenakker et al. ’91, Tanaka et al. ’91, Kolodziej et al. ’91, Feischer et al. ’93] NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

  18. Some history of WW (before ’05) Frontier of higher order lowest order amplitudes for an onshell W-pair calculations at the time [Alles et al. ’77, Gaemers&Gounaris. ’79] electroweak correction to onshell W-pair [Lemione&Veltman ’80, Philippe ’82, Fleischer et al. ’89, Boehm ’88] electroweak correction to onshell W decay [Bardeen et al. ’86, Jegerlehner ’88, Denner&Sack et al. ‘90] inclusion of hard photon radiation [Beenakker et al. ’91, Tanaka et al. ’91, Kolodziej et al. ’91, Feischer et al. ’93] improved Born approximation: include universal corrections (running coupling, ISR, Coulomb singularities) [Dittmaier et al. ’93, Kuroda et al. ’97] NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

  19. Some history of WW (before ’05) Frontier of higher order lowest order amplitudes for an onshell W-pair calculations at the time [Alles et al. ’77, Gaemers&Gounaris. ’79] electroweak correction to onshell W-pair [Lemione&Veltman ’80, Philippe ’82, Fleischer et al. ’89, Boehm ’88] electroweak correction to onshell W decay [Bardeen et al. ’86, Jegerlehner ’88, Denner&Sack et al. ‘90] inclusion of hard photon radiation [Beenakker et al. ’91, Tanaka et al. ’91, Kolodziej et al. ’91, Feischer et al. ’93] improved Born approximation: include universal corrections (running coupling, ISR, Coulomb singularities) [Dittmaier et al. ’93, Kuroda et al. ’97] various DPA approximations: leading term around the poles of the W propagators [Beenakker et al. ’98, Jadach et al. ’01. Denner et al. ’99, Kurihara et al. ’01] NB: this is not a complete list of references Giulia Zanderighi − Four fermion production near the W-pair production threshold 6 /22

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