Multiplicity distributions of gluon and quark jets and tests of QCD analytic predictions

被引:54
作者
Ackerstaff, K [1 ]
Alexander, G
Allison, J
Altekamp, N
Anderson, KJ
Anderson, S
Arcelli, S
Asai, S
Axen, D
Azuelos, G
Ball, AH
Barberio, E
Barlow, RJ
Bartoldus, R
Batley, JR
Baumann, S
Bechtluft, J
Beeston, C
Behnke, T
Bell, AN
Bell, KW
Bella, G
Bentvelsen, S
Bethke, S
Biebel, O
Biguzzi, A
Bird, SD
Blobel, V
Bloodworth, IJ
Bloomer, JE
Bobinski, M
Bock, P
Bonacorsi, D
Boutemeur, M
Bouwens, BT
Braibant, S
Brigliadori, L
Brown, RM
Burckhart, HJ
Burgard, C
Burgin, R
Capiluppi, P
Carnegie, RK
Carter, AA
Carter, JR
Chang, CY
Charlton, DG
Chrisman, D
Clarke, PEL
Cohen, I
机构
[1] CERN, European Org Particle Phys, CH-1211 Geneva 23, Switzerland
[2] Univ Cambridge, Cavendish Lab, Cambridge CB3 0HE, England
[3] Carleton Univ, Dept Phys, Ottawa Carleton Inst Phys, Ottawa, ON K1S 5B6, Canada
[4] Carleton Univ, Ctr Res Particle Phys, Ottawa, ON K1S 5B6, Canada
[5] Univ Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, England
[6] Univ Bologna, Dipartimento Fis, I-40126 Bologna, Italy
[7] Ist Nazl Fis Nucl, I-40126 Bologna, Italy
[8] Univ Bonn, Inst Phys, D-53115 Bonn, Germany
[9] Univ Calif Riverside, Dept Phys, Riverside, CA 92521 USA
[10] Univ Chicago, Enrico Fermi Inst, Chicago, IL 60637 USA
[11] Univ Chicago, Dept Phys, Chicago, IL 60637 USA
[12] Univ Freiburg, Fak Phys, D-79104 Freiburg, Germany
[13] Heidelberg Univ, Inst Phys, D-69120 Heidelberg, Germany
[14] Indiana Univ, Dept Phys, Bloomington, IN 47405 USA
[15] Queen Mary Univ London, London E1 4NS, England
[16] Rhein Westfal TH Aachen, Inst Phys 3, D-52056 Aachen, Germany
[17] UCL, London WC1E 6BT, England
[18] Univ Manchester, Schuster Lab, Dept Phys, Manchester M13 9PL, Lancs, England
[19] Univ Maryland, Dept Phys, College Pk, MD 20742 USA
[20] Univ Montreal, Nucl Phys Lab, Quebec City, PQ H3C 3J7, Canada
[21] Univ Oregon, Dept Phys, Eugene, OR 97403 USA
[22] Rutherford Appleton Lab, Didcot OX11 0QX, Oxon, England
[23] Technion Israel Inst Technol, Dept Phys, IL-32000 Haifa, Israel
[24] Tel Aviv Univ, Dept Phys & Astron, IL-69978 Tel Aviv, Israel
[25] Univ Tokyo, Int Ctr Elementary Particle Phys, Tokyo 113, Japan
[26] Univ Tokyo, Dept Phys, Tokyo 113, Japan
[27] Kobe Univ, Kobe, Hyogo 657, Japan
[28] Brunel Univ, Uxbridge UB8 3PH, Middx, England
[29] Weizmann Inst Sci, Dept Particle Phys, IL-76100 Rehovot, Israel
[30] Univ Hamburg, DESY, Inst Expt Phys 2, D-22607 Hamburg, Germany
[31] Univ Victoria, Dept Phys, Victoria, BC V8W 3P6, Canada
[32] Univ Alberta, Dept Phys, Edmonton, AB T6G 2J1, Canada
[33] Duke Univ, Dept Phys, Durham, NC 27708 USA
[34] Res Inst Particle & Nucl Phys, H-1525 Budapest, Hungary
[35] Inst Nucl Res, H-4001 Debrecen, Hungary
[36] Univ Munich, Sekt Phys, D-85748 Garching, Germany
[37] Univ British Columbia, Dept Phys, Vancouver, BC V6T 1Z1, Canada
[38] TRIUMF, Vancouver, BC V6T 2A3, Canada
[39] Lajos Kossuth Univ, Dept Expt Phys, Debrecen, Hungary
[40] NYU, Dept Phys, New York, NY 10003 USA
来源
EUROPEAN PHYSICAL JOURNAL C | 1998年 / 1卷 / 3-4期
关键词
D O I
10.1007/s100520050097
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
Gluon jets are identified in e(+)e(-) hadronic annihilation events by tagging two quark jets in the same hemisphere of an event. The gluon jet is defined inclusively ns all the particles in the opposite hemisphere. Gluon jets defined in this manlier hale a close correspondence to gluon jets as they are defined for analytic calculations, and are almost independent of a:let finding algorithm. The charged particle multiplicity distribution of the gluon jets is presented, and is analyzed for its mean. dispersion, skew, and curtosis values, and for it factorial and cumulant moments. The results are compared to the analogous results found for a sample of light quark (uds) jets, also defined inclusively. We observe differences between the mean: skew and curtosis values of gluon and quark jets, but not between their dispersions. The cumulant moment results are compared to the predictions of QCD analytic calculations. A calculation which includes next-to-next-to-leading order corrections and energy conservation is observed to provide a much improved description of the data compared to a next-to-leading order calculation without energy conservation. There is agreement between the data and calculation for the ratios of the cumulant moments between gluon and quark jets.
引用
收藏
页码:479 / 494
页数:16
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