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

Constrained MSSM Unification of the gauge couplings Radiative EW Symmetry Breaking Heavy quark and lepton masses Rare decays (b -> sγ, b->μμ) Anomalous magnetic…

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…

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%

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

Basic Operation on Signals Continuous-Time Signals The signal is the actual physical phenomenon that carries information, and the function is a mathematical description of…

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…

ω : angular frequency (radians/s) 0 −A A xc(t) = A cos(2πft) xs(t) = A sin(2πft) = A cos(2πft− π/2) - amplitude A -amplitude A - phase: 0 -phase:

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…

MSSM Higgs  Tau Tau  Leptonic Missing Et and Mass Reconstruction F. Duru, U. Akgun, S. Kunori, Y. Onel The University of Iowa Fermilab F. Duru, APS April Meeting 2006,…

LFV in MSSM based on the minimal SO(10) model Amon Ilakovac Department of Theoretical physics University of Zagreb, Croatia Collaboration Takeshi Fukuyama, Ritsumeikan Univ.,…

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

Bodek-Moriond-EW-2016.pptxPrecision Measurements of Electroweak Parameters with Z Bosons at the Tevatron ( sin2θWeff , sin2θWon-shell, Mw indiret) Rencontres

Microsoft PowerPoint - seminar_ewsb_edit ((FermilabFermilab)) –– prospects and conclusionsprospects and conclusions Bs mixing 22 33 SU(3): SU(3): (QCD)(QCD) W

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