Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at $\sqrt{s}=$ 13 TeV
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[1] Mossolov,et al. Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at s=13 TeV , 2018, Physical Review D.
[2] Yi Wang,et al. Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at √s=13 TeV , 2018, Journal of Instrumentation.
[3] S. M. Etesami,et al. Search for new physics in dijet angular distributions using proton–proton collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} , 2018, The European Physical Journal. C, Particles and Fields.
[4] Atlas Collaboration. Search for new high-mass phenomena in the dilepton final state using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}$ = 13 TeV with the ATLAS detector , 2017, 1707.02424.
[5] V. M. Ghete,et al. Search for narrow resonances in dilepton mass spectra in proton–proton collisions at √s = 13 TeV and combination with 8 TeV data , 2017 .
[6] C. Focke,et al. Color-singlet production at NNLO in MCFM , 2016, The European Physical Journal C.
[7] D. Bourilkov. Exploring the LHC Landscape with Dileptons , 2016, 1609.08994.
[8] A. Manohar,et al. How Bright is the Proton? A Precise Determination of the Photon Parton Distribution Function. , 2016, Physical review letters.
[9] V. Ravindran,et al. NNLO QCD corrections to the Drell–Yan cross section in models of TeV-scale gravity , 2016, 1606.08454.
[10] D. Bourilkov. Photon-induced Background for Dilepton Searches and Measurements in pp Collisions at 13 TeV , 2016, 1606.00523.
[11] J. Huston,et al. PDF4LHC recommendations for LHC Run II , 2015, 1510.03865.
[12] John M. Campbell,et al. A multi-threaded version of MCFM , 2015, The European Physical Journal C.
[13] C. Collaboration,et al. Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at √s = 8 TeV , 2015, 1502.02701.
[14] J. Latorre,et al. Parton distributions for the LHC run II , 2014, 1410.8849.
[15] Peter Skands,et al. An introduction to PYTHIA 8.2 , 2014, Comput. Phys. Commun..
[16] J. T. Childers,et al. Search for contact interactions and large extra dimensions in the dilepton channel using proton–proton collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setl , 2014, The European Physical Journal C.
[17] R. Frederix,et al. The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations , 2014, 1405.0301.
[18] Frank Petriello,et al. Combining QCD and electroweak corrections to dilepton production in the framework of the FEWZ simulation code , 2012 .
[19] S. Forte,et al. Parton distributions with LHC data , 2012, 1207.1303.
[20] Michal Czakon,et al. Top++: A program for the calculation of the top-pair cross-section at hadron colliders , 2011, Comput. Phys. Commun..
[21] J. Campbell,et al. Vector boson pair production at the LHC , 2011, 1105.0020.
[22] J. Huston,et al. The PDF4LHC Working Group Interim Recommendations , 2011, 1101.0538.
[23] E. Re. Single-top Wt-channel production matched with parton showers using the POWHEG method , 2010, 1009.2450.
[24] Alfio Lazzaro,et al. The RooStats Project , 2010, 1009.1003.
[25] N. Kidonakis. Two-loop soft anomalous dimensions for single top quark associated production with a W- or H- , 2010, 1005.4451.
[26] E. Re,et al. A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX , 2010, 1002.2581.
[27] João Paulo Teixeira,et al. The CMS experiment at the CERN LHC , 2008 .
[28] P. Nason,et al. Matching NLO QCD computations with Parton Shower simulations: the POWHEG method , 2007, 0709.2092.
[29] G. Ridolfi,et al. A Positive-weight next-to-leading-order Monte Carlo for heavy flavour hadroproduction , 2007, 0707.3088.
[30] P. Nason. A new method for combining NLO QCD with shower Monte Carlo algorithms , 2004, hep-ph/0409146.
[31] J. Varela,et al. The CMS trigger system , 2004, 1609.02366.
[32] J. Campbell,et al. An update on vector boson pair production at hadron colliders , 1999, hep-ph/9905386.
[33] J. Hewett. Indirect collider signals for extra dimensions , 1998, hep-ph/9811356.
[34] J. Lykken,et al. On Kaluza-Klein states from large extra dimensions , 1998, hep-ph/9811350.
[35] James D. Wells,et al. Quantum Gravity and Extra Dimensions at High-Energy Colliders , 1998, hep-ph/9811291.
[36] Savas Dimopoulos,et al. The Hierarchy problem and new dimensions at a millimeter , 1998, hep-ph/9803315.
[37] V. Barger,et al. Search for Physics Beyond the Standard Model , 1993, hep-ph/9305316.
[38] Estia Eichten,et al. New Tests for Quark and Lepton Substructure , 1983 .
[39] Procedure for the LHC Higgs boson search combination in Summer 2011 , 2011 .
[40] J. Ott,et al. theta – a framework for template-based modeling and inference , 2010 .
[41] A. Dell'Acqua,et al. Geant4—a simulation toolkit , 2003 .
[42] Particle Data Group. Review of Particle Physics , 1998 .
[43] Simone Alioli,et al. Nlo Vector-boson Production Matched with Shower in Powheg Emanuele Re , 2022 .