Abstract
The properties of hadronic jets in ${e}^{+}{e}^{\ensuremath{-}}$ annihilation are examined in quantum chromodynamics, without using the assumptions of the parton model. We find that two-jet events dominate the cross section at high energy, and have the experimentally observed angular distribution. Estimates are given for the jet angular radius and its energy dependence. We argue that the detailed results of perturbation theory for production of arbitrary numbers of quarks and gluons can be reinterpreted in quantum chromodynamics as predictions for the production of jets.
Keywords
Affiliated Institutions
Related Publications
Higgs Bosons from Two-Gluon Annihilation in Proton-Proton Collisions
We estimate the cross section for Higgs-boson production in proton-proton collisions. We find that most of the cross section comes from a two-gluon annihilation process, in whic...
Hadronic molecules
A large number of experimental discoveries especially in the heavy quarkonium\nsector that did not at all fit to the expectations of the until then very\nsuccessful quark model ...
Strong and Electroweak Corrections to the Production of a<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mtext mathvariant="normal">Higgs Boson</mml:mtext><mml:mo>+</mml:mo><mml:mn>2</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mtext mathvariant="normal">Jets</mml:mtext></mml:math>via Weak Interactions at the Large Hadron Collider
Radiative corrections of strong and electroweak interactions are presented at next-to-leading order for the production of a Higgs boson plus two hard jets via weak interactions ...
Enhanced leading production of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="italic">D</mml:mi></mml:mrow><mml:mrow><mml:mo>±</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="italic">D</mml:mi></mml:mrow><mml:mrow><mml:mi mathvariant="normal">*</mml:mi><mml:mo>±</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>in 250 GeV<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">π</mml:mi></mml:mrow><mml:mrow><mml:mo>±</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>-nucleon interactions
A leading charm meson is one with longitudinal momentum fraction, xF>0, whose light quark (or antiquark) is of the same type as one of the quarks in the beam particles. We repor...
Publication Info
- Year
- 1977
- Type
- article
- Volume
- 39
- Issue
- 23
- Pages
- 1436-1439
- Citations
- 736
- Access
- Closed
External Links
Social Impact
Social media, news, blog, policy document mentions
Citation Metrics
Cite This
Identifiers
- DOI
- 10.1103/physrevlett.39.1436