51猎奇入口 of jet shapes in inclusive jet production in pp虅 collisions at s=1.96 TeV
Physical Review D Particles Fields Gravitation and Cosmology 71:11 (2005)
Abstract:
We report on a study of jet shapes in inclusive jet production in pp虅 collisions at s=1.96 TeV using the upgraded collider detector at Fermilab in Run II (CDF II) and based on an integrated luminosity of 170 pb-1. Measurements are carried out on jets with rapidity 0.1<|Yjet|<0.7 and transverse momentum 37GeV/cAn Improved weighting algorithm to achieve software compensation in a fine grained LAr calorimeter.
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 545:3 (2005) Pages 803-812
Measurement of charged-particle multiplicities in gluon and quark jets in pp虅 collisions at 鈭歴 = 1:8 TeV
Physical Review Letters 94:17 (2005)
Abstract:
We report the first largely model independent measurement of charged particle multiplicities in quark and gluon jets, NMeasurements of bottom-antibottom azimuthal production correlations in proton-antiproton collisions at s=1.8TeV
Physical Review D Particles Fields Gravitation and Cosmology 71:9 (2005) 1-39
Abstract:
We have measured the azimuthal angular correlation of bb虅 production, using 86.5pb-1 of data collected by Collider Detector at Fermilab (CDF) in pp虅 collisions at s=1.8TeV during 1994-1995. In high-energy pp虅 collisions, such as at the Tevatron, bb虅 production can be schematically categorized into three mechanisms. The leading-order (LO) process is "flavor creation," where both b and b虅 quarks substantially participate in the hard scattering and result in a distinct back-to-back signal in final state. The "flavor excitation" and the "gluon splitting" processes, which appear at next-leading-order (NLO), are known to make a comparable contribution to total bb虅 cross section, while providing very different opening angle distributions from the LO process. An azimuthal opening angle between bottom and antibottom, 螖, has been used for the correlation measurement to probe the interaction creating bb虅 pairs. The 螖 distribution has been obtained from two different methods. One method measures the 螖 between bottom hadrons using events with two reconstructed secondary vertex tags. The other method uses bb虅鈫�(J/ 蠄X)(X鈥�) events, where the charged lepton () is an electron (e) or a muon (渭), to measure 螖 between bottom quarks. The bb虅 purity is determined as a function of 螖 by fitting the decay length of the J/蠄 and the impact parameter of the. Both methods quantify the contribution from higher-order production mechanisms by the fraction of the bb虅 pairs produced in the same azimuthal hemisphere, ftoward. The measured ftoward values are consistent with both parton shower Monte Carlo and NLO QCD predictions. 漏 2005 The American Physical Society.Search for ZZ and ZW production in pp虅 collisions at s=1.96TeV
Physical Review D Particles Fields Gravitation and Cosmology 71:9 (2005) 1-7