PPT-Associated Top-pair Production with a heavy boson through NNLL+NLO accuracy

Author : bikersjoker | Published Date : 2020-08-27

at the LHC Anna Kulesza University of Münster Rencontres de Moriond QCD amp High Energy Interactions 2330 March 2019 In collaboration with L Motyka D Schwartländer

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Associated Top-pair Production with a heavy boson through NNLL+NLO accuracy: Transcript


at the LHC Anna Kulesza University of Münster Rencontres de Moriond QCD amp High Energy Interactions 2330 March 2019 In collaboration with L Motyka D Schwartländer T Stebel. 1 The Formal Description 2 32 The Informal Description 3 321 Respect each others time 3 322 Be a team player 3 323 Yuta. . Orikasa. (SOKENDAI). Satoshi . Iso. (KEK,SOKENDAI). Nobuchika. Okada(University of Alabama). Phys.Lett.B676(2009)81. Phys.Rev.D80(2009)115007. The Standard Model is the best theory of describing the nature of particle physics, which is in excellent agreement with almost of all current experiments.. (s). Why do we need them?. What do they look like?. Have we found them?. γ. Quantum Electrodynamics. predicts one . massless. . spin-1. . gauge boson. PHOTON. g. Quantum . Chromodynamics. . predicts . 2014. Overview. Review of the Standard Model and the Higgs boson. Creating Higgs bosons. The discovery of a “Higgs-like” particle on July 4, 2012. Is it really the Higgs boson?. The Standard Model. Princeton University. Princeton Plasma Physics Laboratory Colloquium. September . 26, . 2012. Is it the Higgs Boson?. Many Princeton undergraduate students have worked on the CMS experiment over the years. Tim Wiser. Splash P2506. 3 Nov 2012. Plan . Standard Model of Particle Physics. Particles, interactions, and the Higgs field. Drawing Feynman diagrams. These simple pictures are actually . calculational. flavor . produced in association with W and Z bosons. Pierre-Hugues Beauchemin. o. n behalf of the ATLAS Collaboration. Tufts University. ICHEP2012 -Melbourne, Australia . 0. 5/07/2012. Outline. Context of the measurements. G. Heinrich, J. . Huston. , J. . Maestre. , D. . Maitre. , R. . . Pittau. ,. G. . Soyez. (jet . liason. ). Understanding cross sections at the LHC. PDF. ’. s, PDF luminosities. and PDF uncertainties. 10. th. International Spring Seminar on Nuclear Physics Vietri . sul. Mare, Italy, May 21-25. K. Nomura (U. Tokyo). collaborators: . T. Otsuka, N. Shimizu (U. Tokyo), and L. Guo (RIKEN). Interacting Boson Model (IBM) and its microscopic basis. Caroline Steiblin. Prof. Al . Goshaw. Dr. Andrea . Bocci. Duke University. 1. Purpose. C. omparing . Monte-Carlo (MC) simulations of Z boson mass reconstruction from . muons. , photons, and electrons . -Yan. 1. 2. Anna’s calculations for correlation function . DY+hadron. . are based on arXiv:. 1204.4861 and the following process. which is NLO to process a) so are b) and c). see Anna’s paper arXiv:1008.2652. December 12th-16th, 2011. Table of Contents. CERN Higgs boson Flash Report. . Executive Summary & Findings 3-4. Background 5. Pre-announcement overview 6. Announcement overview 7. In particle physics , elementary particles and forces give rise to the world around us.. The two main elementary particles which form the major constituent of matter are the LEPTONS and QUARKS.. Quark+Quark=hadrons [protons&neutrons].. (and elsewhere). Michael Schmitt (Northwestern University). LOOPFEST 13: June 18, . 2014. Topics. June 17, 2014. 2. Vector Boson Production at CMS (and elsewhere).

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