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
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
References(35)
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