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Cross Section for b Jet Production in pbar-p Collisions at sqrt(s) = 1.8 TeV

D0 collaboration, B. Abbott

Abstract

Bottom quark production in pbar-p collisions at sqrt(s)=1.8 TeV is studied with 5 inverse picobarns of data collected in 1995 by the DO detector at the Fermilab Tevatron Collider. The differential production cross section for b jets in the central rapidity region (|y(b)| < 1) as a function of jet transverse energy is extracted from a muon-tagged jet sample. Within experimental and theoretical uncertainties, DO results are found to be higher than, but compatible with, next-to-leading-order QCD predictions.

Cross Section for b Jet Production in pbar-p Collisions at sqrt(s) = 1.8 TeV

Abstract

Bottom quark production in pbar-p collisions at sqrt(s)=1.8 TeV is studied with 5 inverse picobarns of data collected in 1995 by the DO detector at the Fermilab Tevatron Collider. The differential production cross section for b jets in the central rapidity region (|y(b)| < 1) as a function of jet transverse energy is extracted from a muon-tagged jet sample. Within experimental and theoretical uncertainties, DO results are found to be higher than, but compatible with, next-to-leading-order QCD predictions.

Paper Structure

This paper contains 1 equation, 3 figures, 1 table.

Figures (3)

  • Figure 1: Fraction of muon-tagged jets which come from b decays. $E_T$ is the calorimeter-only component (see text) of the $b$ jet transverse energy.
  • Figure 2: Differential cross section for $b$ jet production.
  • Figure 3: Integrated cross section for $b$ quark production.