Energy helps accuracy: Electroweak precision tests at hadron colliders

We show that high energy measurements of Drell–Yan at the LHC can serve as electroweak precision tests. Dimension-6 operators, from the Standard Model Effective Field Theory, modify the high energy behavior of electroweak gauge boson propagators. Existing measurements of the dilepton invariant mass spectrum, from neutral current Drell–Yan at 8 TeV, have comparable sensitivity to LEP. We propose measuring the transverse mass spectrum of charged current Drell–Yan, which can surpass LEP already with 8 TeV data. The 13 TeV LHC will elevate electroweak tests to a new precision frontier.

[1]  Pavel Strachota,et al.  Measurement of the inclusive W± and Z/γ∗ cross sections in the e and μ decay channels in pp collisions at √s=7TeV with the ATLAS detector , 2012 .

[2]  M. Grazzini,et al.  Vector boson production at hadron colliders: a fully exclusive QCD calculation at next-to-next-to-leading order. , 2009, Physical review letters.

[3]  Kirill Melnikov,et al.  Dilepton rapidity distribution in the Drell-Yan process at next-to-next-to-leading order in QCD. , 2003, Physical review letters.

[4]  Alessandro Strumia,et al.  Minimal Dark Matter , 2006 .

[5]  S. Forte,et al.  Parton distributions with QED corrections , 2013, 1308.0598.

[6]  M. Z. Mehta,et al.  Search for new physics in final states with a lepton and missing transverse energy in pp collisions at the LHC , 2013 .

[7]  S. Chatrchyan,et al.  Search for contact interactions in $$ events in $pp$ collisions at $s=7$ TeV , 2012 .

[8]  R. Contino,et al.  Effective field theory analysis of double Higgs boson production via gluon fusion , 2015 .

[9]  A. Pomarol,et al.  Probing the standard model with dijets at the LHC , 2012, 1201.6510.

[10]  S. M. Etesami,et al.  Measurements of differential and double-differential Drell–Yan cross sections in proton–proton collisions at $$\sqrt{s} = 8$$s=8$$\,\text {TeV}$$TeV , 2015, The European physical journal. C, Particles and fields.

[11]  Enrico Morgante,et al.  On the validity of the effective field theory for dark matter searches at the LHC part III: analysis for the t-channel , 2013, 1409.6668.

[12]  Riccardo Barbieri,et al.  Electroweak symmetry breaking after LEP1 and LEP2 , 2004, hep-ph/0405040.

[13]  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.

[14]  J. T. Childers,et al.  Search for contact interactions and large extra dimensions in dilepton events from pp collisions at √s=7 TeV with the ATLAS detector , 2013 .

[15]  L. Dixon,et al.  High-precision QCD at hadron colliders: Electroweak gauge boson rapidity distributions at next-to-next-to leading order , 2003, hep-ph/0312266.

[16]  Massimiliano Grazzini,et al.  Next-to-next-to-leading-order subtraction formalism in hadron collisions and its application to Higgs-boson production at the large hadron collider. , 2007, Physical review letters.

[17]  M. Dorigo,et al.  Precise measurement of the W-boson mass with the CDF II detector. , 2012, Physical review letters.

[18]  T. Tuuva,et al.  Measurement of the inclusive W and Z production cross sections in pp collisions at $ \sqrt {s} = 7 $ TeV with the CMS experiment , 2011 .

[19]  Julija Šukys,et al.  Erratum , 2011 .

[20]  M. Pérez-Victoria,et al.  Vector triplets at the LHC , 2013, 1307.2589.

[21]  R. K. Shivpuri,et al.  Measurement of the W boson mass with the D0 detector. , 2012, Physical review letters.

[22]  Frank Petriello,et al.  Combining QCD and electroweak corrections to dilepton production in the framework of the FEWZ simulation code , 2012 .

[23]  I-A Melzer-Pellmann,et al.  Measurement of inclusive W and Z boson production cross sections in pp collisions at sqrt[s] = 8 TeV. , 2014, Physical review letters.

[24]  Roelof Hamberg,et al.  A complete calculation of the order αs2 correction to the Drell-Yan K-factor , 1991 .

[25]  M. Kraemer,et al.  Vices and virtues of Higgs effective field theories at large energy , 2014, 1406.7320.

[26]  Kaven Henry Yau Wong,et al.  Measurement of $W^{\pm}$ and $Z$-boson production cross sections in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector , 2016 .

[27]  Sidney D. Drell,et al.  Massive Lepton-Pair Production in Hadron-Hadron Collisions at High Energies , 1970 .

[28]  M. Kramer,et al.  Radiative corrections to W -boson hadroproduction: Higher-order electroweak and supersymmetric effects , 2007, 0710.3309.

[29]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[30]  S. Forte,et al.  Parton distributions with LHC data , 2012, 1207.1303.

[31]  D. Wyler,et al.  Effective lagrangian analysis of new interactions and flavour conservation , 1986 .

[32]  Ye Li,et al.  FEWZ 2.0: A code for hadronic Z production at next-to-next-to-leading order , 2010, Comput. Phys. Commun..

[33]  K. Melnikov,et al.  Electroweak gauge boson production at hadron colliders through O(alpha(s)**2) , 2006, hep-ph/0609070.

[34]  Andrea Benaglia,et al.  Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at √s=8 TeV , 2015 .

[35]  J. Blas,et al.  Global constraints on lepton-quark contact interactions , 2013, 1307.5068.

[36]  Takeuchi,et al.  New constraint on a strongly interacting Higgs sector. , 1990, Physical review letters.