'Tevatron' diaporamas de présentation

Summary and Conclusions

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Lighting up the Higgs sector with photons at CDF

Lighting up the Higgs sector with photons at CDF. Fermilab Joint Experimental-Theoretical Seminar. Karen Bland for the CDF collaboration May 20, 2011. Tevatron and CDF Performance. Thanks to accelerator division for delivering luminosity! And CDF for keeping the detector running well!

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Information and treatment of unknown correlations in BLUE combinations

Information and treatment of unknown correlations in BLUE combinations. Andrea Valassi (CERN IT-ES) Roberto Chierici (IPN Lyon) Top LHC Working Group, 29 th November 2012. Motivation. Best Linear Unbiased Estimators (BLUE) are widely used for precision measurement combinations

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Beam -Beam Interactions

CERN Accelerator School Chavannes de Bogis , Switzerland 8 November 2013. Beam -Beam Interactions. Tatiana Pieloni (BE -ABP- ICE) Thanks to W. Herr. Hadron Circular Colliders. Bunch intensity:. Transverse Beam size :. Number of bunches. Revolution frequency.

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Now have <pile-up> ~ 14 per bunch crossing. a challenge for tracking and for low- p T jets!

ATLAS status report: a snapshot after reaching L = 3.3 10 33 cm -2 s -1 (18 months and 3.2 fb -1 after first collisions at 7 TeV ). Now have <pile-up> ~ 14 per bunch crossing. a challenge for tracking and for low- p T jets!.

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SUSY Studies @Hadron Colliders

SUSY Studies @Hadron Colliders. MSSM and need for models e.g. SUGRA. Limits from Tevatron. SUSY studies at LHC: inclusive analysis and discovery limits. exclusive analysis and precision measurements. Gauge Mediated SB models R parity violating models. SUSY Higgs sector Conclusions.

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Higgs & SUSY Phenomenology

Higgs & SUSY Phenomenology. Nikos Konstantinidis. Plan. Motivation & Introduction to SUSY Further reading: S.P.Martin, hep-ph/9709356 SUSY Higgs Further reading: Spira & Zerwas, hep-ph/9803257 Higgs & SUSY Higgs phenomenology at hadron colliders (esp. LHC)

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Weak Mixing Angle and Higgs Mass in Gauge-Higgs Unification Models with Brane Kinetic Terms

Weak Mixing Angle and Higgs Mass in Gauge-Higgs Unification Models with Brane Kinetic Terms. 2012. 2. 21 @YongPyong2012 Jubin Park. Collaboration with Prof. Sin Kyu Kang and Prof. We-Fu Chang. arXiv:1111.5422 [ hep -ph] submitted to JHEP . Contents.

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LHCb results

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Highlights from Top Quark Physics

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Intensity ramp-up

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PVDIS at 11 GeV with SoLID

PVDIS at 11 GeV with SoLID. (g A e g V T + ? g V e g A T ). g V is a function of sin 2 ? W. to. PV Electron Scattering. Continuous interplay between probing hadron structure and electroweak physics. Parity-violating electron scattering has become a precision tool.

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Base-Band Tune (BBQ) Measurement System Marek Gasior Beam Instrumentation Group, CERN

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Searching for the light Higgs Boson with light at the Tevatron

Searching for the light Higgs Boson with light at the Tevatron. Callie DeMay Craig Group and Raymond Culbertson. Fermi National Accelerator Laboratory. Chain of Five Accelerators Last Chain = 4 mile Tevatron Protons and antiprotons collide head on at 1.96 TeV

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Les Houches 05, session 2

Les Houches 05, session 2. BSM-SUSY, experimental. EGRET point. Philippe Gris, Lauren Tompkins, Dirk Zerwas. m 0 =1400 GeV m 1/2 = 180 GeV A 0 =700 GeV tan ? = 51 ? > 0. Tevatron Perspective:. 10 fb -1. 2 fb -1. 30 fb -1.

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High Energy Physics at U T A

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Lecture 3 - Magnets and Transverse Dynamics I

Lecture 3 - Magnets and Transverse Dynamics I. ACCELERATOR PHYSICS Lecture 3 Longitudinal Motion TT 2012 E. J. N. Wilson. Physics of the electron v. protons . When we collide Protons we collide complex assemblies of three quarks Only two quarks interact

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Physics 434 Module 4 week 2: the FFT

Physics 434 Module 4 week 2: the FFT. Explore Fourier Analysis and the FFT. Exploration VI. The resonance function. Note that this is the response function to driving the system at a frequency ?. Now, go discrete!.

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Introduction

Introduction. Roberto Chierici ( CERN/CNRS), Maria Costa (IFIC Valencia), Markus Cristinziani (Bonn / CERN), Roberto Tenchini (INFN/Pisa) on behalf of the TOPLHCWG. First open TOPLHCWG workshop CERN, 19 July 2012. Motivation. Large sample of top quarks at the LHC

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Current Statistical Issues in Particle Physics

Current Statistical Issues in Particle Physics. Louis Lyons Particle Physics Oxford U.K. Future of Statistical Theory

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