We calculate the O (α s 2) corrections to the event shape in e+ e− annihilation due to the
parton processes e+ e−→ qq G, e+ e−→ qq qq and e+ e−→ qq GG. The event shape is …

Nuclear Physics B187 (1981) 301-320 O North-Holland Publishing Company PERTURBATIVE
QCD CALCULATION OF JET CROSS SECTIONS IN e+e Page 1 Nuclear Physics B187 (1981) …

Order α <SUP>2</SUP><SUB>S</SUB> correction to jet cross sections in e <SUP>+</SUP>e
<SUP>-</SUP> annihilation - NASA/ADS Now on home page ads icon ads Enable full ADS …

We investigate some infrared stable properties of jets in e+ e− annihilation that receive their
first contribution in QCD perturbation theory at second order in the strong coupling constant …

We calculate the two-jet cross section in order α s 2 in the framework of massless
perturbative QCD, using for jet resolution the jet mass. We derive results for two different …

We have calculated the four-jet production processes e+ e−→ qq gg and e+ e−→ qqqq to
lowest-order QCD perturbation theory. We find that (qqqq) production is small compared to …

We investigate the four-jet production processes e+ e−→ qq gg and e+ e−→ qq qq in lowest
order QCD perturbation theory. We estimate that four-jet events should be detectable at a …

We present a new class of observables which distinguish events containing two or three
hadron jets from those containing a larger number. These observables, which essentially …

COMMENT ON THE O(ats 2) CORRECTIONS TO JET-PRODUCTION IN e+e -
ANNIHILATION Deutsches Elektronen-S3,nchrotron DESY, Hamburg, Ger Page 1 Volume …

We give perturbative predictions for the distribution of the C-parameter event shape variable
in e+ e− annihilation, including resummation of large logarithms in the two-jet (small-C) …