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Electroweak Theory and Higgs Physics Preliminary Version Chris Quigg Fermilab Theory Group [email protected] Fermilab Academic Lectures · 1 – 17 November 2005 Chris Quigg…

The Standard Model (Electroweak Theory)NEΣTP Institute · Pylos, Greece Chris Quigg Electroweak Theory · Pylos 2002 1 Tentative Outline . . . Sources of

[email protected] Chris Quigg Electroweak Theory · Fermilab Academic Lectures 2005 1bis [Z, e+e−, pp, νN , (g − 2)µ, . . . ]

Nessun titolo diapositiva LHC Physics Luca Lista INFN - Napoli Electroweak results 1 p p W±, Z, γ* l ± l ∓, νl (−) q q(´) − EWK processes at LHC LHC Physics Measurement…

Giant Steps Chris Quigg Fermilab [email protected] Low-Emittance Muon Collider Workshop · 12 February 2007 mailto:[email protected] A Decade of Discovery Past . . . EW theory…

4. Conclusions 1. Introduction sin2 θlept eff = 0.23150 ± 0.00016 0.07% ΓZ[ GeV] = 2.4952 ± 0.0023 0.09% MZ[ GeV] = 91.1875 ± 0.0021 0.002%

Perspectives in High-Energy Physics Chris Quigg Theoretical Physics Department Fermi National Accelerator Laboratory quigg@fnalgov • Neutrino Puzzles • The World’s…

Nuclear and Particle Physics Franz Muheim 1 Standard Model Standard Model -- ElectroweakElectroweak InteractionsInteractions Weak Neutral Interactions Neutral Currents NC…

Electroweak physics at LHC Marina Cobal, University of Udine ‘IFAE’, Torino Apr 14 - Apr 16, 2004 Outline Introduction W mass measurement Top mass measurement EW single…

Electroweak Physics Lecture 2 Last Lecture Use EW Lagrangian to make predictions for width of Z boson: Relate this to what we can measure: σ(e+e−→ff) Lots of extracted…

Electroweak Physics Lecture 3 Status so far… 6 parameters out of 18 Today 7 more! The Grand Reckoning Correlations of all yesterday’s Z peak observables from all 4 LEP…

Electroweak Precision Measurements: Today The Electroweak Sector of the SM § EW sector described by 3 parameters @ tree-level » g,g’ Coupling constants of

Hadron Collider Physics: Measurement Search Discovery at the High-Energy Frontier Chris Quigg Fermilab Benasque · March 7 – 11 2005 A Decade of Discovery Past � Electroweak…

Electroweak results at the Tevatron Susana Cabrera for the CDF and D0 collaborations XXIIth International Workshop on Deep-Inelastic Scattering Electroweak Physics at Run…

Electroweak results at the Tevatron Susana Cabrera for the CDF and D0 collaborations XXIIth International Workshop on Deep-Inelastic Scattering Electroweak Physics at Run…

PRELIMINARY SHIP DESIGN PARAMETER ESTIMATION START Read : owner’s requirements (ship type dwt/TEU, speed) Define limits on L, B, D, T Define stability constraints First…

1. 100 101 102 103 Eγ [GeV] 10−7 E2 dN/dE[GeVcm−2 s−1 ] 2 × 10−8 MDM = 42.39 GeV, χ2 = 58.26, σv = 6.82 × 10−27 2. 100 101 102 103 Eγ [GeV] 10−7 E2 dN/dE[GeVcm−2…

DOG Preliminary pcb LAYOUT Seraj Dosenbach Greg Lammers Beau Morrison Ananya Panja Printed Circuit Board Layout Narrative plus Preliminary PCB Layout 1 PCB LAYOUT 3.45 inches…

Electroweak Baryogenesis K Funakubo Saga Univ June 4 ‘04 @ KEK Baryon Asymmetry of the Universe nB s ≡ nb − nb̄ s � 037 − 088 × 10−10 1 Big Bang Nucleosynthesis…

LHC Signals of MSSM Electroweak Baryogenesis David Morrissey Department of Physics University of Michigan Michigan Center for Theoretical Physics MCTP With: Csaba Balázs…