Phys. Rev. D
76,
012005
(2007)
[12 pages]
Comparison of particle production in quark and gluon fragmentation at √s∼10 GeV
R. A. Briere et al. CLEO Collaboration
Show All Authors/Affiliations
Hide All Authors/Affiliations
R. A. Briere1, T. Ferguson1, G. Tatishvili1, H. Vogel1, M. E. Watkins1, J. L. Rosner2, N. E. Adam3, J. P. Alexander3, D. G. Cassel3, J. E. Duboscq3, R. Ehrlich3, L. Fields3, R. S. Galik3, L. Gibbons3, R. Gray3, S. W. Gray3, D. L. Hartill3, B. K. Heltsley3, D. Hertz3, C. D. Jones3, J. Kandaswamy3, D. L. Kreinick3, V. E. Kuznetsov3, H. Mahlke-Krüger3, P. U. E. Onyisi3, J. R. Patterson3, D. Peterson3, J. Pivarski3, D. Riley3, A. Ryd3, A. J. Sadoff3, H. Schwarthoff3, X. Shi3, S. Stroiney3, W. M. Sun3, T. Wilksen3, M. Weinberger3, S. B. Athar4, R. Patel4, V. Potlia4, J. Yelton4, P. Rubin5, C. Cawlfield6, B. I. Eisenstein6, I. Karliner6, D. Kim6, N. Lowrey6, P. Naik6, M. Selen6, E. J. White6, J. Wiss6, R. E. Mitchell7, M. R. Shepherd7, D. Besson8, H. K. Swift8,*, T. K. Pedlar9, D. Cronin-Hennessy10, K. Y. Gao10, J. Hietala10, Y. Kubota10, T. Klein10, B. W. Lang10, R. Poling10, A. W. Scott10, A. Smith10, P. Zweber10, S. Dobbs11, Z. Metreveli11, K. K. Seth11, A. Tomaradze11, J. Ernst12, K. M. Ecklund13, H. Severini14, W. Love15, V. Savinov15, O. Aquines16, Z. Li16, A. Lopez16, S. Mehrabyan16, H. Mendez16, J. Ramirez16, G. S. Huang17, D. H. Miller17, V. Pavlunin17, B. Sanghi17, I. P. J. Shipsey17, B. Xin17, G. S. Adams18, M. Anderson18, J. P. Cummings18, I. Danko18, D. Hu18, B. Moziak18, J. Napolitano18, Q. He19, J. Insler19, H. Muramatsu19, C. S. Park19, E. H. Thorndike19, F. Yang19, T. E. Coan20, Y. S. Gao20, M. Artuso21, S. Blusk21, J. Butt21, J. Li21, N. Menaa21, G. C. Moneti21, R. Mountain21, S. Nisar21, K. Randrianarivony21, R. Sia21, T. Skwarnicki21, S. Stone21, J. C. Wang21, K. Zhang21, G. Bonvicini22, D. Cinabro22, M. Dubrovin22, A. Lincoln22, D. M. Asner23, and K. W. Edwards23 (CLEO Collaboration)
1Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA 2Enrico Fermi Institute, University of Chicago, Chicago, Illinois 60637, USA 3Cornell University, Ithaca, New York 14853, USA 4University of Florida, Gainesville, Florida 32611, USA 5George Mason University, Fairfax, Virginia 22030, USA 6University of Illinois, Urbana-Champaign, Illinois 61801, USA 7Indiana University, Bloomington, Indiana 47405, USA 8University of Kansas, Lawrence, Kansas 66045, USA 9Luther College, Decorah, Iowa 52101, USA 10University of Minnesota, Minneapolis, Minnesota 55455, USA 11Northwestern University, Evanston, Illinois 60208, USA 12State University of New York at Albany, Albany, New York 12222, USA 13State University of New York at Buffalo, Buffalo, New York 14260, USA 14University of Oklahoma, Norman, Oklahoma 73019, USA 15University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA 16University of Puerto Rico, Mayaguez, Puerto Rico 00681 17Purdue University, West Lafayette, Indiana 47907, USA 18Rensselaer Polytechnic Institute, Troy, New York 12180, USA 19University of Rochester, Rochester, New York 14627, USA 20Southern Methodist University, Dallas, Texas 75275, USA 21Syracuse University, Syracuse, New York 13244, USA 22Wayne State University, Detroit, Michigan 48202, USA 23Carleton University, Ottawa, Ontario, Canada K1S 5B6
Received 19 April 2007; published 27 July 2007
Using e+e-→hadrons data collected with the CLEO-III detector at the Cornell Electron Storage Ring, we study the inclusive production of baryons/antibaryons (p,Λ) and mesons (ϕ and f2(1270)) in gluon-fragmentation and quark-fragmentation processes. We first corroborate previous per-event total particle yields in Υ(1S)→ggg compared with nearby continuum (e+e-→qq̅ ) indicating greater (∼×2) per-event yields of baryons in 3-gluon fragmentation. We find similar results when we extend that comparison to include the Υ(2S) and Υ(3S) resonances. With higher statistics, we now also probe the momentum dependence of these per-event particle yields. Next, we compare particle production in the photon-tagged process Υ(1S)→ggγ with that in e+e-→qq̅ γ events, to allow comparison of two-parton with three-parton particle-specific fragmentation. For each particle, we determine the “enhancement” ratio, defined as the ratio of particle yields per gluon-fragmentation event compared to quark-fragmentation event. Thus defined, an enhancement of 1.0 implies equal per-event production in gluon and quark fragmentation. In the photon-tagged analysis (Υ(1S)→ggγ compared to e+e-→qq̅ γ), we find almost no enhancement for protons (∼1.2±0.1), but a significant enhancement (∼1.9±0.3) for Λ’s. This small measured proton enhancement rate is supported by a study of baryon production in χb2→gg→p+X relative to χb1→qq̅ g→p+X. Overall, per-event baryon production in radiative two-gluon fragmentation is somewhat smaller than that observed in three-gluon decays of the Υ(1S). Our results for baryon production are inconsistent with the predictions of the JETSET (7.3) fragmentation model.
© 2007 The American Physical Society
URL:
http://link.aps.org/doi/10.1103/PhysRevD.76.012005
DOI:
10.1103/PhysRevD.76.012005
PACS:
12.38.Aw, 12.38.Qk, 13.60.Hb, 13.87.Fh
*Current address: Department of Physics, University of California, Berkeley, Berkeley, CA 94720-7300, USA
|
|