Single weak boson production at TeV e+ e- colliders

Dec, 1990
53 pages
Published in:
  • Nucl.Phys.B 365 (1991) 544-596
  • Published: 1991
Report number:
  • KEK-TH-255,
  • KEK-PREPRINT-90-40,
  • DTP-90-82,
  • HUPD-9015,
  • UT-574-TOKYO,
  • MAD-PH-417

Citations per year

199119992007201520230246810
Abstract: (Elsevier)
We present exact tree level matrix elements for all the single weak boson production processes to order e 3 in very high energy e + e − collisions; e + e − → e ± v (−) c W ∓ , e + e − Z , v c v c Z and γγZ. The electron mass is kept finite so that the differential and total cross sections are accurate up to terms of order m e 2 / s . The weak boson distributions are compared with those obtained by the equivalent photon/electron approximation (EPA), which works reasonably well at high vector boson transverse momenta but fails at small transverse momenta for the processes e + e − → e + e − Z and γγZ. A simple modification of the EPA formulae is found to give a reasonable overall description of the distributions for all the single weak boson production processes. Electron helicity-flip amplitudes are found to contribute at the percent level at most, which can be reproduced accurately by a novel collinear approximation with equivalent real photon or electron distributions in an electron. Interference effects between the annihilation and non-annihilation diagrams are found to be significant only below the weak boson pair production threshold. Also explained is a straightforward method to incorporate the leptonic and parton level hadronic decays of the weak bosons into the production amplitudes.
  • electron positron: annihilation
  • annihilation: electron positron
  • electron positron: inelastic scattering
  • inelastic scattering: electron positron
  • intermediate boson: electroproduction
  • electroproduction: intermediate boson
  • differential cross section
  • channel cross section: energy dependence
  • tree approximation
  • equivalent photon approximation