TY - JOUR
T1 - Charged multiplicities in Z decays into u, d and s quarks
AU - Abbiendi, G
AU - Anagnostou, Georgios
AU - Bloodworth, Ian
AU - Bright-Thomas, Paul
AU - Charlton, David
AU - Hawkes, Christopher
AU - Homer, Roger
AU - Jimack, Martin
AU - Jovanovic, Predrag
AU - Lloyd, Alun
AU - McMahon, Thomas
AU - O'Neale, Stephen
AU - Talbot, Scott
AU - Watson, Miriam
AU - Watkins, Peter
AU - Watson, Alan
AU - Watson, Nigel
AU - Wilson, John
PY - 2001/2/1
Y1 - 2001/2/1
N2 - About 4.4 million hadronic decays of Z bosons, recorded by the OPAL detector at LEP at a centre-of-mass energy of around roots = 91.2 GeV, are used to determine the mean charged particle multiplicities for the three light quark flavours. Events from primary u, d, and s quarks are tagged by selecting characteristic particles which carry a large fraction of the beam energy. The charged particle multiplicities are measured in the hemispheres opposite to these particles. An unfolding procedure is applied to obtain these multiplicities for each primary light quark flavour. This yields [n(u)] = 17.77 +/- 0.51(-1.20)(+0.86), [n(d)] = 21.44 +/- 0.63(-1.17)(+1.46), [n(s)] = 20.02 +/- 0.13(-0.37)(+0.39), where statistical and systematic errors are given. The results for [n(u)] and [n(d)] are almost fully statistically anti-correlated. Within the errors the result is consistent with the flavour independence of the strong interaction for the particle multiplicities in events from the light up, down, and strange quarks.
AB - About 4.4 million hadronic decays of Z bosons, recorded by the OPAL detector at LEP at a centre-of-mass energy of around roots = 91.2 GeV, are used to determine the mean charged particle multiplicities for the three light quark flavours. Events from primary u, d, and s quarks are tagged by selecting characteristic particles which carry a large fraction of the beam energy. The charged particle multiplicities are measured in the hemispheres opposite to these particles. An unfolding procedure is applied to obtain these multiplicities for each primary light quark flavour. This yields [n(u)] = 17.77 +/- 0.51(-1.20)(+0.86), [n(d)] = 21.44 +/- 0.63(-1.17)(+1.46), [n(s)] = 20.02 +/- 0.13(-0.37)(+0.39), where statistical and systematic errors are given. The results for [n(u)] and [n(d)] are almost fully statistically anti-correlated. Within the errors the result is consistent with the flavour independence of the strong interaction for the particle multiplicities in events from the light up, down, and strange quarks.
U2 - 10.1007/s100520100611
DO - 10.1007/s100520100611
M3 - Article
SN - 1434-6044
VL - 19
SP - 257
EP - 268
JO - European Physical Journal C
JF - European Physical Journal C
IS - 2
ER -