We review two approaches to calculate the next-to-leading order cross section for the inclusive production of charm quarks using either massive or massless quarks. We discuss the massless limit derived from the massive theory. This limit differs from the genuine massless version with MS factorizatio
Measurement of the inclusive D∗± production in γγ collisions at LEP
✍ Scribed by J. Heß; A. Ngac
- Publisher
- Elsevier Science
- Year
- 2004
- Tongue
- English
- Weight
- 648 KB
- Volume
- 126
- Category
- Article
- ISSN
- 0920-5632
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✦ Synopsis
The inclusive production of D** mesons in two-photon collisions is measured with the ALEPH detector at e+e-centre-of-mass energies from 183 GeV to 209 GeV. A total of 360 i 27 D*' meson events are observed from an integrated luminosity of 699 pb-'. Cont$>tions from direct and single-resolved processes are separated using the ratio of the transverse momentum p, of the D** to the visible invariant mass Wyis of the event. Differential cross sections of D** production as functions of pf** and the pseudorapidity (qD** ( are measured in the range 2GeV/c < pt *** < 12 GeV/c and IqD**/ < 1.5. They are compared to next-to-leading order (NLO) perturbative QCD calculations. The extrapolation of the integrated visible D** cross section to the total charm cross section, based on the Pythia Monte Carlo program, yields u(e+e--+ efe-cF)(fi))=leiGev = 731 i 74,tat k 47,,,t + 157,,t, pb.
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