Rising Bosonic Electroweak Virtual Effects at High Energy e+e- Colliders

Abstract

The virtual massive gauge boson effects on several observables in the process of charged fermion pairs production at $e^{+}{e}^{-}$ colliders are computed up to the TeV energy range in the Standard Model, working in the ``$Z$-peak subtracted'' representation. It is shown that these effects increase regularly with energy, approaching the typical ten percent relative size. A careful numerical evaluation is proposed, where the conditions dictated by gauge invariance are consistently implemented.

REVTeX, 21 pages, 11 figures. Minor changes, misprints corrected, conclusions unchanged. To appear in Phys. Rev. D

References in corpus (4)

• Physics with e^+e^- Linear Colliders
• Analytic approach to the complete set of QED corrections to fermion pair production in e+e- annihilation
• General constraints on light resonances in a strongly coupled symmetry breaking sector
• Signals for Neutralino Box Effects at LEP2

Cited by in corpus (42)

• Weak Corrections are Relevant for Dark Matter Indirect Detection
• Next-to-Next-to-Leading Logarithms in Four-Fermion Electroweak Processes at High Energy
• Two-loop electroweak angular-dependent logarithms at high energies
• Electroweak corrections to Wγand Zγproduction at the LHC
• Next-to-leading-order electroweak corrections to the production of four charged leptons at the LHC
• Two-Loop Electroweak Logarithms in Four-Fermion Processes at High Energy
• Two-Loop Sudakov Form Factor in a Theory with Mass Gap
• Two-loop electroweak next-to-leading logarithmic corrections to massless fermionic processes
• The Two Loop Crossed Ladder Vertex Diagram with Two Massive Exchanges
• NLO QCD and electroweak corrections to $Z+\gamma$ production with leptonic Z-boson decays
• Logarithmic expansion of electroweak corrections to four-fermion processes in the TeV region
• Next-to-leading mass singularities in two-loop electroweak singlet form factors
• Two-Loop Electroweak Logarithms
• NLO QCD and electroweak corrections to W+γ production with leptonic W-boson decays
• Electroweak Sudakov Logarithms and Real Gauge-Boson Radiation in the TeV Region
• The role of the top mass in b-production at future lepton colliders
• Anomalous triple-gauge-boson interactions in vector-boson pair production with RECOLA2
• TeV scale Dark Matter and electroweak radiative corrections
• NLO QCD+NLO EW corrections to diboson production matched to parton shower
• The two-loop vector form factor in the Sudakov limit
• The role of universal and non universal Sudakov logarithms in four fermion processes at TeV energies: the one-loop approximation revisited
• Electroweak corrections and anomalous triple gauge-boson couplings in WW and WZ production at the LHC
• One-loop electroweak Sudakov logarithms: a revisitation and automation
• An algorithm for the high-energy expansion of multi-loop diagrams to next-to-leading logarithmic accuracy
• Logarithmic electroweak corrections to e+ e- -> nue anti-nue W+ W-
• Next-to-leading-order electroweak corrections to the production of three charged leptons plus missing energy at the LHC
• Automation of electroweak corrections for LHC processes
• Electroweak double-logs at small x
• Infrared weak corrections to strongly interacting gauge bosons scattering
• Four lepton production and the accuracy of QED FSR
• Anomalous Sudakov Form Factors
• On electroweak corrections to neutral current Drell-Yan with the POWHEG BOX
• Logarithmic EW corrections at one-loop
• Probing the weak mixing angle at high energies at the LHC and HL-LHC
• Weak effects in b-jet production at hadron colliders
• Z-peak subtracted representation of Bhabha scattering and search for new physics effects
• Supersymmetric structure of electroweak Sudakov corrections
• Electroweak corrections to b-jet and di-jet production
• Hard processes in multi-TeV ion collisions
• Bounds on universal new physics effects from fermion-antifermion production at LEP2
• Yukawa enhanced electroweak corrections at high energy in the MSSM
• Higgs Boson Exchange Effects in $l^{+}{l}^{-}\to W^{+}{W}^{-}$ at High Energy