2002
DOI: 10.1016/s0370-2693(02)02088-9
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Analysis of fluctuation of fluctuations in 32S–AgBr interactions at 200 AGeV

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Cited by 47 publications
(29 citation statements)
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“…The erraticity analysis of hadronic interaction at 250 GeV/c in the NA22 experiment [40] confirms the dominance of statistical fluctuations in the experimental measurement. In emulsion experiments [12,41], the experimental data on AB interactions were found to be far apart from the MC-generated results and (or) results generated by purely statistical considerations, an observation that is similar to the present analysis.…”
Section: The Erraticitysupporting
confidence: 69%
“…The erraticity analysis of hadronic interaction at 250 GeV/c in the NA22 experiment [40] confirms the dominance of statistical fluctuations in the experimental measurement. In emulsion experiments [12,41], the experimental data on AB interactions were found to be far apart from the MC-generated results and (or) results generated by purely statistical considerations, an observation that is similar to the present analysis.…”
Section: The Erraticitysupporting
confidence: 69%
“…In meson-proton collisions at 250 GeV/c beam momentum, it was found that the erracticity measures are dominated by statistical fluctuations at such low energy [26]. In nucleus-nucleus collisions interesting signals have been found both in models [27] and in emulsion experiments [28] even at low energies. At high energy where we can examine the deconfinement-to-confinement transition, it will become clear in the next section, where model calculations can generate concrete local multiplicity fluctuations, that it is more comprehensive to consider the range 1 ≤ p ≤ 2 in the study of C p,q (M ).…”
Section: Moments For Event-by-event Fluctuationsmentioning
confidence: 99%
“…[11] we have chosen 730 events of 16 O-AgBr interactions at 2.1A GeV [10]. The emission angle and azimuthal angle are measured for each track by taking readings of the coordinates of the interaction point ͑X 0 , Y 0 , Z 0 ͒, coordinates ͑X 1 , Y 1 , Z 1 ͒ at the end of the linear portion of each secondary track, and coordinate ͑X i , Y i , Z i ͒ of a point on the incident beam.…”
mentioning
confidence: 99%