Search for gluinos and scalar quarks in pp̄ Collisions at √s = 1.8 TeV using the missing energy plus multijets signature
Physical Review Letters 88:4 (2002) 418011-418016
Abstract:
A search for gluinos and scalar quarks in a data sample of 84 pb -1 of pp̄ collisions at √s = 1.8 TeV was performed. The final state of large missing transverse energy and three or more jets was investigated. The data was compared with predictions of constrained supersymmetric models and gluinos masses below 195 GeV/c 2, independent of the squark mass were excluded.Search for charmless B --> VV decays.
Phys Rev Lett 88:2 (2002) 021802
Abstract:
We have studied two-body charmless decays of the B meson into the final states rho(0)rho(0), K(*0)rho(0), K(*0)K(*0), K(*0)K(*0), K(*+)rho(0), K(*+)K(*0), and K(*+)K(*-) using only decay modes with charged daughter particles. Using 9.7x10(6) BB pairs collected with the CLEO detector, we place 90% confidence level upper limits on the branching fractions (1.4-14.1)x10(-5), depending on final state and polarization.Comparison of the Isolated Direct Photon Cross Sections in $p \bar p$ Collisions at $\sqrt{s}=1.8$ TeV and $\sqrt{s}=0.63$ TeV
ArXiv hep-ex/0201004 (2002)
Charged jet evolution and the underlying event in proton-antiproton collisions at 1.8 TeV
Physical Review D Particles Fields Gravitation and Cosmology 65:9 (2002)
Abstract:
The growth and development of “charged particle jets” produced in proton-antiproton collisions at [Formula Presented] are studied over a transverse momentum range from [Formula Presented] [Formula Presented] to [Formula Presented] [Formula Presented] A variety of leading (highest transverse momentum) charged jet observables are compared with the QCD Monte Carlo models HERWIG, ISAJET, and PYTHIA. The models describe fairly well the multiplicity distribution of charged particles within the leading charged jet, the size of the leading charged jet, the radial distribution of charged particles and transverse momentum around the leading charged jet direction, and the momentum distribution of charged particles within the leading charged jet. The direction of the leading “charged particle jet” in each event is used to define three regions of [Formula Presented] space. The “toward” region contains the leading “charged particle jet”, while the “away” region, on the average, contains the away-side jet. The “transverse” region is perpendicular to the plane of the hard [Formula Presented]-to-[Formula Presented] scattering and is very sensitive to the “underlying event” component of the QCD Monte Carlo models. HERWIG, ISAJET, and PYTHIA with their default parameters do not describe correctly all the properties of the “transverse” region. © 2002 The American Physical Society.Correlated inclusive ΛΛ̄ production in e +e- annihilations at √s∼10.5 GeV
Physical Review D 66:5 (2002)