Search for pair production of vector-like quarks in the bWbW channel from proton–proton collisions at √s =13 TeV

[1]  P. D. Luckey,et al.  Cross Section Measurement of t -Channel Single Top Quark Production in pp Collisions at √s = 13 TeV , 2017 .

[2]  C. Collaboration,et al.  Particle-flow reconstruction and global event description with the CMS detector , 2017, 1706.04965.

[3]  Khachatryan,et al.  Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV , 2016, 1607.03663.

[4]  Scoap,et al.  Measurement of the tt¯ production cross section using events in the eμ final state in pp collisions at s=13TeV , 2016, 1611.04040.

[5]  S. M. Etesami,et al.  Search for vectorlike charge 2/3 T quarks in proton-proton collisions at √(s) = 8 TeV , 2016 .

[6]  J. Baglio.  Next-To-Leading Order QCD Corrections to Associated Production of a SM Higgs Boson with a Pair of Weak Bosons in the POWHEG-BOX , 2015, 1512.05787.

[7]  Andrea Benaglia,et al.  Measurement of the differential cross section for top quark pair production in pp collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin} , 2015, The European Physical Journal. C, Particles and Fields.

[8]  Atlas Collaboration.  Search for production of vector-like quark pairs and of four top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector , 2015, 1505.04306.

[9]  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.

[10]  J. Latorre,et al.  Parton distributions for the LHC run II , 2014, 1410.8849.

[11]  Peter Skands,et al.  An introduction to PYTHIA 8.2 , 2014, Comput. Phys. Commun..

[12]  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.

[13]  G. Soyez,et al.  Soft drop , 2014, 1402.2657.

[14]  J. A. Aguilar-Saavedra,et al.  Handbook of vectorlike quarks: Mixing and single production , 2013, 1306.0572.

[15]  A. Mitov,et al.  Total top-quark pair-production cross section at hadron colliders through O(αS(4)). , 2013, Physical review letters.

[16]  P. D. Luckey,et al.  Performance of CMS muon reconstruction in pp collision events at √s = 7 TeV , 2012 .

[17]  Jing Shu,et al.  General composite Higgs models , 2012, 1205.0770.

[18]  M. Cacciari,et al.  FastJet user manual , 2011, 1111.6097.

[19]  C. Collaboration,et al.  Determination of Jet Energy Calibration and Transverse Momentum Resolution in CMS , 2011, 1107.4277.

[20]  R. Mohapatra,et al.  Gauged flavor group with left-right symmetry , 2011, 1103.4170.

[21]  J. S. Conway,et al.  Incorporating Nuisance Parameters in Likelihoods for Multisource Spectra , 2011, 1103.0354.

[22]  E. Re,et al.  A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX , 2010, 1002.2581.

[23]  João Paulo Teixeira,et al.  The CMS experiment at the CERN LHC , 2008 .

[24]  M. Cacciari,et al.  The anti-$k_t$ jet clustering algorithm , 2008, 0802.1189.

[25]  M. Cacciari,et al.  The Catchment Area of Jets , 2008, 0802.1188.

[26]  P. Nason,et al.  Matching NLO QCD computations with Parton Shower simulations: the POWHEG method , 2007, 0709.2092.

[27]  Paul Langacker,et al.  Theory and phenomenology of exotic isosinglet quarks and squarks , 2007, 0708.2701.

[28]  M. Cacciari,et al.  Pileup subtraction using jet areas , 2007, 0707.1378.

[29]  M. Cacciari,et al.  Dispelling the N3 myth for the kt jet-finder , 2005, hep-ph/0512210.

[30]  D. Ankerst,et al.  Kendall's Advanced Theory of Statistics, Vol. 2B: Bayesian Inference , 2005 .

[31]  Hsin-Chia Cheng,et al.  Top partners in little Higgs theories with T-parity , 2005, hep-ph/0510225.

[32]  M. Schmaltz,et al.  LITTLE HIGGS THEORIES , 2005, hep-ph/0502182.

[33]  P. Nason.  A new method for combining NLO QCD with shower Monte Carlo algorithms , 2004, hep-ph/0409146.

[34]  H. Logan,et al.  Loop induced decays of the little Higgs: H ---> gg, gamma gamma , 2003, hep-ph/0302188.

[35]  M. Schmaltz.  Physics beyond the standard model (Theory): Introducing the Little Higgs , 2002, hep-ph/0210415.

[36]  A. Nelson,et al.  The Littlest Higgs , 2002, hep-ph/0206021.

[37]  Enrico Fermi Institute,et al.  Beautiful mirrors and precision electroweak data , 2001, hep-ph/0109097.

[38]  Hsin-Chia Cheng.  Electroweak symmetry breaking and extra dimensions , 1999, hep-ph/9912343.

[39]  Véronique Lefébure,et al.  CMS Simulation Software Using Geant4 , 1999 .

[40]  L. Randall,et al.  A Large mass hierarchy from a small extra dimension , 1999, hep-ph/9905221.

[41]  S. Snyder.  Measurement of the top quark mass at D0 , 1996 .

[42]  M. Kendall,et al.  Kendall's advanced theory of statistics , 1995 .

[43]  G. Kane,et al.  Vector-like fermion and standard Higgs production at hadron colliders☆ , 1990 .

[44]  F. James.  Statistical Methods in Experimental Physics , 1973 .

[45]  Identification of b quark jets at the CMS Experiment in the LHC Run 2 , 2016 .

[46]  A. Dell'Acqua,et al.  Geant4—a simulation toolkit , 2003 .

[47]  Particle Data Group.  Review of Particle Physics , 1998 .