1996
DOI: 10.1016/0370-2693(95)01435-7
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Transverse momentum spectra of charged particles in collisions at

Abstract: We h a v e analysed a sample of 2.36 million minimum bias events produced in pp collisions at p s = 630 GeV in the UA1 experiment at the CERN collider. We h a v e studied production of charged particles with transverse momenta (p T) up to 25 GeV/c. The results are in agreement with QCD predictions. The rise of hp T i with charged particle multiplicity m a y be related to changing production of low p T particles.

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Cited by 49 publications
(30 citation statements)
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“…4.1 that the charged particle multiplicity per participant (both at midrapidity and integrated over all solid angle) is larger in A+A than in p+p at the same energy. At √ s values of 200 GeV and above, it is known that the p T spectra in p+p events with higher than average total multiplicity fall off less steeply than those for minimum bias events [163,164,165]. It should be stressed that we do not claim that an alternative p+p reference spectra is in any way inherently more appropriate.…”
Section: Comparison Of Au+au and Other Systemsmentioning
confidence: 81%
See 1 more Smart Citation
“…4.1 that the charged particle multiplicity per participant (both at midrapidity and integrated over all solid angle) is larger in A+A than in p+p at the same energy. At √ s values of 200 GeV and above, it is known that the p T spectra in p+p events with higher than average total multiplicity fall off less steeply than those for minimum bias events [163,164,165]. It should be stressed that we do not claim that an alternative p+p reference spectra is in any way inherently more appropriate.…”
Section: Comparison Of Au+au and Other Systemsmentioning
confidence: 81%
“…It should be noted that, although the relative yield at low and high p T changes with multiplicity in p+p collisions, there is evidence that the change in shape is relatively small above p T ∼2 GeV/c [165]. In addition, the question of what p+p reference spectrum to use does not affect modification factors such as R Npart P C which directly compare A+A at different centralities.…”
Section: Comparison Of Au+au and Other Systemsmentioning
confidence: 99%
“…Comparison with the AFS [25], UA1 [7], UA1 MIMI [8], and CDF [9] data is made, and the difference between the computed and measured spectra is quantified in terms of a factor K = dσ exp /dσ th LO . We have extracted the K-factors and their √ s-dependence from the highest transverse momenta of the measured spectra.…”
Section: Discussionmentioning
confidence: 99%
“…Unfortunately, we are not aware of useful identified hard meson production data from pp or pp reactions at energies above √ s ≈ 60 GeV; we have total hadron production data in the form of (h + + h − )/2 from CERN UA1 [13][14][15] and the Tevatron CDF [16]. Since the production of hadrons other than kaons and pions (in particular protons and antiprotons) increases with energy, the accuracy of the extraction of k 2 T decreases with increasing energy.…”
Section: Extension To Rhic Energiesmentioning
confidence: 99%
“…Higher energies are less thoroughly explored, with mostly calorimetric data on total hadron production (in lieu of the identified pion and kaon spectra at lower energies). In the present paper, we use CERN UA1 [13][14][15] and Tevatron CDF [16] data from pp → h ± reactions to bracket the RHIC energy range from above. The presence of nuclear effects modifies the predictions of the pQCD-improved parton model for hard particle production in pA collisions, as indicated by available pA hadron production data [6,7,11,17,18].…”
Section: Introductionmentioning
confidence: 99%