Lecture Notes in Physics
DOI: 10.1007/3-540-07866-5_17
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On the phenomenology of multihadron production in e+e− annihilation

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Cited by 2 publications
(3 citation statements)
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“…In Ref [4] three parametrizations were used, i.e. < N ch > = a·s b inspired by the fireball and hydrodinamical models for hadron-hadron interactions [11], empirical expression used in the analysis of p + p data [12] < N ch > = a + b·s + c·lns 2 and < N ch > = a + b·exp[c ln(s/Q 2 0 )] [10] and it was shown that they give similar values for χ 2 /d.o.f. if the fits do not include energies lower than 5 GeV.…”
Section: Charged Particle Multiplicity In Heavy Ion Central Collisionsmentioning
confidence: 99%
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“…In Ref [4] three parametrizations were used, i.e. < N ch > = a·s b inspired by the fireball and hydrodinamical models for hadron-hadron interactions [11], empirical expression used in the analysis of p + p data [12] < N ch > = a + b·s + c·lns 2 and < N ch > = a + b·exp[c ln(s/Q 2 0 )] [10] and it was shown that they give similar values for χ 2 /d.o.f. if the fits do not include energies lower than 5 GeV.…”
Section: Charged Particle Multiplicity In Heavy Ion Central Collisionsmentioning
confidence: 99%
“…Energy scaling of the pseudo-rapidity charged particle density in central rapidity as a function of centrality One of the observables which are sensitive to the particle production mechanism and partonic structure of the colliding objects is the charged particle density and its dependence on the collision geometry. Detailed information on centrality dependence of charged particle density at midrapidity in A + A collisions exists starting from AGS [13,14], at SPS [15,16] and RHIC [11], [17]- [23] energies. The systematic compilation of these results [23] and the recent data from ALICE Collaboration at 2.76 TeV [24] are represented in Fig.2.…”
Section: Charged Particle Multiplicity In Heavy Ion Central Collisionsmentioning
confidence: 99%
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