Abstract:The scaled factorial moment, which is a statistical tool for measuring large local fluctuations of dynamical origin, has been utilized to probe the distribution of secondary particles produced in 16 O-AgBr interactions at 60 GeV/n. The analysis indicates the occurrence of a non-thermal phase transition in case of pionisation in heavy-ion interactions at extremely high energy.
“…The data sets used in the present analysis were obtained by irradiating Ilford-G5 emulsion stacks (a) by an 16 O beam with incident energy 60 GeV/nucleon and (b) by an 32 S beam with incident energy 200 GeV/nucleon at CERN, SPS [18,19].…”
An analysis of data of pions emitted from ultra-relativistic nuclear interactions initiated by 16 O-AgBr at 60 GeV/nucleon and 32 S-AgBr at 200 GeV/nucleon reveals the existence of emission asymmetry in the azimuthal plane which is found to depend on the number of pions but to be nearly independent of projectile mass and energy.
“…The data sets used in the present analysis were obtained by irradiating Ilford-G5 emulsion stacks (a) by an 16 O beam with incident energy 60 GeV/nucleon and (b) by an 32 S beam with incident energy 200 GeV/nucleon at CERN, SPS [18,19].…”
An analysis of data of pions emitted from ultra-relativistic nuclear interactions initiated by 16 O-AgBr at 60 GeV/nucleon and 32 S-AgBr at 200 GeV/nucleon reveals the existence of emission asymmetry in the azimuthal plane which is found to depend on the number of pions but to be nearly independent of projectile mass and energy.
“…Now let us look at multiparticle production in heavy-ion collisions from this point of view. In a recent paper [10] the intermittency phenomenon for the distribution of secondary particles produced in 16 O-AgBr interactions at 60 GeV/n was studied using the scaled factorial moments. In fig.…”
mentioning
confidence: 99%
“…3 we show the data represented in ref. [10] for the pseudorapidity (filled circles) and for the azimuthal (open circles) phase spaces in the case of largest bin regions. As in the previous figures the axes are chosen for comparison with the stretched lognormal distribution (30) (straight lines, the best fit, are drawn to indicate agreement between the data and representation (30)).…”
mentioning
confidence: 99%
“…Fig.3ζp/p vs. p1/3 for the data obtained at ultrarelativistic heavy-ion collisions (for secondary particles produced in 16 O-AgBr interactions at 60 GeV/n)[10]. Filled circles correspond to the pseudorapidity and open circles correspond to the azimuthal phase spaces.…”
Analytic branching cascades are suggested to interpret the experimental data obtained in e + e − annihilation into hadrons and in ultrarelativistic heavy-ion collisions. The branching dimension extracted from these data using normalized factorial moments (both for one-and two-dimensional cases and for rapidity and azimuthal phase spaces) turned out to be universal and equal to 2. The universal character of this phenomenon is emphasized by the fact that the same branching dimension d = 2 turned out to be relevant also to data obtained in a laboratory experiment on the branching cascades in the fluid turbulence.
An investigation of non-statistical fluctuations in 16
O-AgBr interaction at 60A GeV in terms of factorial correlators is presented. The correlated moments are found to increase with decreasing bin-bin separation D
, following a power law.
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