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Blue: background uncertainty Background + DMA signal describe EGRET data! Blue: WIMP mass uncertainty Wim de Boer, Karlsruhe LHC-D, SUSY/BSM, Bonn, Feb. 23, 2007 * Analysis…
Slide 1Martin zur Nedden, HU Berlin 1 WS 2007/08: Physik am LHC 5. Higgs Searches The Higgs-mechanism in the SM Yukava-coupling, masses of fermions Higgs Production: Searches…
Seiberg duality for SUSY QCD Phases of gauge theories Coulomb : V R ∼ 1R Free electric : V R ∼ 1R lnRΛ Free magnetic : V R ∼ lnRΛR Higgs : V R ∼ constant Confining…
SUSY UED LHT at the LHC Howard Baer Florida State University of Oklahoma ⋆ SUSY at LHC • SUSY signatures • SM backgrounds • cuts: optimizing signalBG • LHC reach…
Looking for SUSY Dark Matter with ATLAS The Story of a Lonely Lepton Nadia Davidson Supervisor: Elisabetta Barberio The Standard Model In high agreement with experimental…
SUSY (s)lepton flavour studies with ATLAS Iris Borjanovic University of Lecce Flavour in the era of the LHC, 7-10 November, CERN Outline mSUGRA Sleptons Fast simulation studies…
SUSY-Sumrules and MT2 Combinatorics David Curtin bla arXiv:1004.5350, arXiv:1102(?).???? In Collaboration with Maxim Perelstein, Monika Blanke bla Cornell Institute for High…
PowerPoint 24th Jan. 17 CiRfSE WS 1 New physics searches in Z + MET events 24th Jan. 17 CiRfSE WS 2 Ex.) : Z + invisible particles Run-1 Z O(10) X Run-1 Higgs-portal model
Introduction to Lattice Supersymmetry Simon Catterall Syracuse University Introduction to Lattice Supersymmetry – p. 1 Motivation Motivation: SUSY theories - cancellations…
Podivnost na LHC Supervisor: Jana Crkovská J. Krejčí, R. Mahdal, A. Miklíková, J. Mrázek, T. Novotný, L. Polcar Podivné částice __ 0 _ _ _ _ Rozpady Ξ-→π- Λ→…
Podivnost na LHC Supervisor: Jana Crkovská J. Krejčí, R. Mahdal, A. Miklíková, J. Mrázek, T. Novotný, L. Polcar Podivné částice __ 0 _ _ _ _ Rozpady Ξ-→π- Λ→…
b− τ Yukawa Unification in SUSY SU5 with Mirage Mediation: LHC and Dark Matter Implications Shabbar Razaa,1, Qaisar Shafib,2 and Cem Salih Ünc, 3 aDepartment of Physics,…
SUSY gauge theories SUSY QCD Consider a SUSY SUN with F “flavors” of “quarks” and squarks Qi = φi QiFi i = 1 F where φ is the squark and Q is the quark Qi = φi…
Stefano Redaelli, CERN, BE-ABP for the Collimation Project and HL-LHC-WP5 teams The LHC Collimation Baseline for HL-LHC 3rd Joint HiLumi LHC-LARP Annual Meeting November…
1. Σπύρος Ευστ. Τζαμαρίας Φυσική και Τεχνολογίαστα μεγάλα πειράματα του CERNμε τον επιταχυντή LHC…
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…
Yedekler * * Bora Akgün - CMU, V. Erkcan Özcan - UCL Candidate for W en * Bora Akgün - CMU, V. Erkcan Özcan - UCL 7 TeV’de bir muon * Bora Akgün - CMU, V. Erkcan…
Quarkonia production at LHC Preliminary FAMOS results on signal and CMSSW_1_2_0 Gobinda Majumder India-CMS meeting 21-22 Jan 2007 Onium production at LHC : ckin(3)=5 σ(J/ψ)*Br(μμ)=653…
γ*, Z and W production at LHCb Ronan McNulty, LHCEWWG, 5.04.2011 1 AFB at LHC Myfanwy Liles (University of Liverpool) Ronan McNulty (University College Dublin) Tara Shears…
SUSY Lagrangians Wess-Zumino The free Wess–Zumino model S = ∫ d4x Ls + Lf Ls = ∂µφ∗∂µφ Lf = iψ†σµ∂µψ gµν = ηµν = diag1−1−1−1 φ→ φ+ δφ…