Study of gluon versus quark fragmentation in [Formula presented] and [Formula presented] events at [Formula presented]=10 GeV
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Alam, M S
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Athar, S B
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Ling, Z
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Mahmood, A H
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Severini, H
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Timm, S
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Wappler, F
a
Anastassov, A
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Blinov, S
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Duboscq, J E
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Fujino, D
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Fulton, R
b
Gan, K K
b
Hart, T
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Honscheid, K
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Kagan, H
b
Kass, R
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Lee, J
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Spencer, M B
b
Sung, M
b
Undrus, A
b
Wanke, R
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Wolf, A
b
Zoeller, M M
b
Nemati, B
c
Richichi, S J
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Ross, W R
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Skubic, P
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Wood, M
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Bishai, M
d
Fast, J
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Gerndt, E
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Hinson, J W
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Menon, N
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Miller, D H
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Shibata, E I
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Shipsey, I P J
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Yurko, M
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Gibbons, L
e
Johnson, S D
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Kwon, Y
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Roberts, S
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Thorndike, E H
e
Jessop, C P
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g
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h
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h
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h
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h
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h
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h
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Greene, R
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Perera, L P
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Barish, B
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Chadha, M
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Chan, S
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Eigen, G
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Miller, J S
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Grady, C O’
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Schmidtler, M
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Urheim, J
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Weinstein, A J
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Wurthwein F
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Asner, D M
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Bliss, D W
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Brower, W S
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Masek, G
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Paar, H P
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Sivertz, M
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Gronberg, J
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Kutschke, R
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Lange, D J
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Menary, S
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Morrison, R J
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Nakanishi, S
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Nelson, H N
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Nelson, T K
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Qiao, C
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Richman, J D
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Roberts, D
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Ryd, A
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Tajima, H
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Witherell, M S
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Balest, R
o
Behrens, B H
o
Cho, K
o
Ford, W T
o
Park, H
o
Rankin, P
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Roy, J
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Smith, J G
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Alexander, J P
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Bebek, C
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Berger, B E
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Berkelman, K
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Bloom, K
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Cassel, D G
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Cho, H A
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Coffman, D M
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Crowcroft, D S
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Dickson, M
p
Drell, P S
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Ecklund, K M
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Ehrlich, R
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Elia, R
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Foland, A D
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Gaidarev, P
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Galik, R S
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Gittelman, B
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Gray, S W
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Hartill, D L
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Heltsley, B K
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Hopman, P I
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Jones, S L
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Kandaswamy, J
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Katayama, N
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Kim, P C
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Kreinick, D L
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Lee, T
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Liu, Y
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Ludwig, G S
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Masui, J
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Mevissen, J
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Mistry, N B
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Ng, C R
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Nordberg, E
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Ogg, M
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Patterson, J R
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Peterson, D
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Riley, D
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Soffer, A
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Ward, C
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Athanas, M
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Avery, P
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Jones, C D
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Lohner, M
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Prescott, C
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Yang, S
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Yelton, J
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Zheng, J
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Brandenburg, G
r
Briere, R A
r
Gao, Y S
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Kim, D Y J
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Wilson, R
r
Yamamoto, H
r
Browder, T E
s
Li, F
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Li, Y
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Rodriguez, J L
s
Bergfeld, T
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Eisenstein, B I
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Ernst, J
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Gladding, G E
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Gollin, G D
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Hans, R M
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Johnson, E
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Karliner, I
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Marsh, M A
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Palmer, M
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Selen, M
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Thaler, J J
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Edwards, K W
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Bellerive, A
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Janicek, R
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MacFarlane, D B
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McLean, K W
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Patel, P M
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Sadoff, A J
v
Ammar, R
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Baringer, P
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Bean, A
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Besson, D
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Coppage, D
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Darling, C
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Davis, R
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Hancock, N
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Kotov, S
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Kravchenko, I
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Kwak, N
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Anderson, S
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Kubota, Y
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Lattery, M
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O'Neill J J
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Patton, S
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Poling, R
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Riehle, T
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Savinov, V
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Smith, A
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The backgrounds from “merged” (Formula presented)’s are, at these energies, negligible due to the good resolution of the CLEO-II detector. See, for example, N. Hancock, “Determination of the Strong Coupling Constant from Radiative Decays of the (Formula presented)(1S) Meson”, thesis, University of Kansas, 1996 (unpublished), for a fuller discussion of the merged (Formula presented) backgrounds
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The backgrounds from “merged” (Formula presented)’s are, at these energies, negligible due to the good resolution of the CLEO-II detector. See, for example, N. Hancock, “Determination of the Strong Coupling Constant from Radiative Decays of the (Formula presented)(1S) Meson”, thesis, University of Kansas, 1996 (unpublished), for a fuller discussion of the merged (Formula presented) backgrounds.
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DELPHI Collaboration, J. Fuster and S. Martí (private communication), and presented at QCD 1996, Montepellier, France;, Fuster and Martí predict (Formula presented) for (Formula presented)=10 GeV. They do not extrapolate as low as the energies probed in this measurement, however
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DELPHI Collaboration, J. Fuster and S. Martí (private communication), and presented at QCD 1996, Montepellier, France;Fuster and Martí predict (Formula presented) for (Formula presented)=10 GeV. They do not extrapolate as low as the energies probed in this measurement, however.
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