Transverse-momentum distributions of charged particles produced inp¯pinteractions at √s¯=630 and 1800 GeV

Abe, F.; Amidei, D.; Apollinari, G.; Ascoli, G.; Ataç, M.; Auchincloss, P.; Baden, A.; Barbaro-Galtieri, A.; Barnes, V. E.; Bedeschi, F.; Belforte, S.; Bellettini, G.; Bellinger, J.; Bensinger, J. R.; Beretvas, A.; Bergé, P.; Bertolucci, S.; Bhadra, S.; Binkley, M.; Blair, R. E.; Blocker, C.; Bofill, J.; Booth, A. W.; Brandenburg, G.; Brown, D.; Byon, A.; Byrum, K. L.; Campbell, M.; Carey, Robert M.; Carithers, W.; Carlsmith, D.; Carroll, J. T.; Cashmore, R. J.; Cervelli, F.; Chadwick, K.; Chapin, T. J.; Chiarelli, G.; Chinowsky, W.; Cihangir, S.; Cline, D.; Connor, D.; Contreras, M.; Cooper, J.; Cordelli, M.; Curatolo, M.; Day, C.; Delfabbro, R.; Dell’Orso, M.; Demortier, L.; Devlin, T.; DiBitonto, D.; Diebold, R.; Dittus, F.; Divirgilio, A.; Elias, J. E.; Ely, R.; Errede, S.; Esposito, B.; Feldman, A.; Flaugher, B.; Focardi, E.; Foster, G. W.; Franklin, M.; Freeman, J.; Frisch, H.; Fukui, Y.; Garfinkel, A. F.; Giannetti, P.; Giokaris, N.; Giromini, P.; Gladney, L.; Gold, M.; Goulianos, K.; Grosso-Pilcher, C.; Haber, C.; Hahn, S. R.; Handler, R.; Harris, R. M.; Hauser, J.; Hessing, T. L.; Hollebeek, R.; Holloway, L.; Hu, P.; Hubbard, B.; Hurst, P.; Huth, J.; Jensen, H.; Johnson, R. P.; Joshi, U.; Kadel, R. W.; Kamon, T.; Kanda, S.; Kardelis, D. A.; Karliner, I.; Kearns, E.; Kephart, R.; Kesten, P.; Keutelian, H.; Kim, S.; Kirsch, L.; Kondo, K.; Kruse, U.; Kuhlmann, S. E.; Laasanen, A. T.; Li, W.; Liss, T. M.; Lockyer, N. S.; Marchetto, F.; Markeloff, R.; Markosky, L. A.; McIntyre, P.; Menzione, A.; Meyer, T. C.; Mikamo, S.; Miller, Michael L.; Mimashi, T.; Miscetti, S.; Mishina, M.; Miyashita, S.; Mondal, N. K.; Mori, Shigeki; Morita, Y.; Mukherjee, A.; Newman-Holmes, C.; Nodulman, L.; Paoletti, R.; Para, A.; Patrick, J.; Phillips, T. J.; Piekarz, H.; Plunkett, R.; Pondrom, L.; Proudfoot, J.; Punzi, G.; Quarrie, D. R.; Ragan, K.; Redlinger, G.; Rhoades, J.; Rimondi, F.; Ristori, L.; Rohaly, T.; Roodman, A.; Sansoni, A.; Sard, R. D.; Scarpine, V.; Schlabach, P.; Schmidt, E.; Schoessow, P.; Schub, M. H.; Schwitters, R. F.; Scribano, A.; Segler, S.; Sekiguchi, M.; Sestini, P.; Shapiro, M.; Sheaff, M.; Shibata, Masayuki; Shochet, M. J.; Siegrist, J.; Sinervo, P.; Skarha, J.; Smith, D.; Snider, F. D.; Denis, R. St.; Stefanini, A.; Takaiwa, Y.; Takikawa, K.; Tarem, S.; Theriot, D.; Tollestrup, A.; Tonelli, G.; Tsay, Y.; Ukegawa, F.; Underwood, D. G.; Vidal, R.; Wagner, R. G.; Wagner, R. L.; Walsh, J.; Watts, T.; Webb, Richard; Westhusing, T.; White, S.; Wicklund, A. B.; Williams, H. H.; Yamanouchi, T.; Yamashita, A.; Yasuoka, K.; Yeh, G. P.; Yoh, J.; Zetti, F.

doi:10.1103/physrevlett.61.1819

Cited by 196 publications

(98 citation statements)

References 19 publications

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“…Here, κ 2,3 are scale factors that are related to the number of quark participants and hence the fraction of the available c.m energy that contributes to particle production. Figure 1c gives the expression [53], ALICE [49], CDF [54], UA1 [55] and UA5 [50]. The error bars include the available systematic uncertainties.…”

Section: Discussionmentioning

confidence: 99%

Scaling Properties of the Mean Multiplicity and Pseudorapidity Density in e−+e+, e±+p, p( p ¯ )+p, p+A and A+A(B) Collisions

et al. 2018

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The charged-particle pseudorapidity density (dN ch /dη) for p(p)+p, p+A and A+A(B) collisions and the mean multiplicity N ch for e − +e + , e ± +p, and p(p)+p collisions are studied for a wide range of beam energies ( √ s). Characteristic scaling patterns are observed for both dN ch /dη and N ch , consistent with a thermal particle production mechanism for the bulk of the soft particles created in all of these systems. The scaling patterns found also validate an essential role for quark participants in these collisions. The measured values for dN ch /dη and N ch are observed to factorize into contributions that depend on log( √ s) and the number of nucleon or quark participant pairs N pp . The quantification of these contributions gives expressions that serve to systematize dN ch /dη and N ch measurements spanning nearly 4 orders of magnitude in √ s and to predict their values as a function of √ s and N pp .

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Section: Discussionmentioning

confidence: 99%

Scaling Properties of the Mean Multiplicity and Pseudorapidity Density in e−+e+, e±+p, p( p ¯ )+p, p+A and A+A(B) Collisions

et al. 2018

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“…Data of other experiments are taken from refs. [22,[31][32][33]. The curve shows the fit to the data points of the form p T = 0.425−0.0197 ln(s)+ 0.00156 ln 2 (s) with p T in GeV/c and s in GeV 2 .…”

Section: Jhep02(2010)041mentioning

confidence: 99%

Transverse-momentum and pseudorapidity distributions of charged hadrons in pp collisions at $\sqrt{s} = 0.9 $ and 2.36 TeV

Khachatryan

Sirunyan²,

Tumasyan³

et al. 2010

J. High Energ. Phys.

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284

227

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Measurements of inclusive charged-hadron transverse-momentum and pseudorapidity distributions are presented for proton-proton collisions at √ s = 0.9 and 2.36 TeV. The data were collected with the CMS detector during the LHC commissioning in December 2009. For non-single-diffractive interactions, the average charged-hadron transverse momentum is measured to be 0.46 ± 0.01 (stat.) ± 0.01 (syst.) GeV/c at 0.9 TeV and 0.50 ± 0.01 (stat.) ± 0.01 (syst.) GeV/c at 2.36 TeV, for pseudorapidities between −2.4 and +2.4. At these energies, the measured pseudorapidity densities in the central region, dN ch /dη| |η|<0.5 , are 3.48 ± 0.02 (stat.) ± 0.13 (syst.) and 4.47 ± 0.04 (stat.) ± 0.16 (syst.), respectively. The results at 0.9 TeV are in agreement with previous measurements and confirm the expectation of near equal hadron production in pp and pp collisions. The results at 2.36 TeV represent the highest-energy measurements at a particle collider to date.

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“…The c.m. energy evolution of the charged hadron pseudorapidity density at η = 0 predicted by the different models in the range √ s = 10 GeV-800 TeV is presented in figure 3 compared to the existing NSD (left panel) and inelastic (right panel) data measured at SppS (UA1 [63], and UA5 [64]), Tevatron (CDF [69,70]) and LHC (ALICE [71][72][73], ATLAS [65] and CMS [66][67][68] Figure 3. Evolution of the charged particle pseudorapidity density at midrapidity, dN ch /dη| η=0 , as a function of collision energy, √ s, for non-single diffractive (left) and inelastic (right) p-p collisions.…”

Section: Inelastic P-p Cross Sectionmentioning

confidence: 99%

Global properties of proton-proton collisions at s = 100 $$ \sqrt{\mathrm{s}}=100 $$ TeV

d’Enterria

Pierog

2016

J. High Energ. Phys.

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Abstract:The global properties of the final states produced in hadronic interactions of protons at centre-of-mass energies of future hadron colliders (such as FCC-hh at CERN, and SppC in China), are studied. The predictions of various Monte Carlo (MC) event generators used in collider physics (pythia 6, pythia 8, and phojet) and in ultrahighenergy cosmic-rays studies (epos, and qgsjet) are compared. Despite their different underlying modeling of hadronic interactions, their predictions for proton-proton (p-p) collisions at √ s = 100 TeV are quite similar. The average of all MC predictions (except phojet) for the different observables are: (i) p-p inelastic cross sections σ inel = 105 ± 2 mb; (ii) total charged multiplicity N ch = 150 ± 20; (iii) charged particle pseudorapidity density at midrapidity dN ch /dη| η=0 = 9.6 ± 0.2; (iv) energy density at midrapidity dE/dη| η=0 = 13.6 ± 1.5 GeV, and dE/dη| η=5 = 670 ± 70 GeV at the edge of the central region; and (v) average transverse momenta at midrapidities p T = 0.76 ± 0.07 GeV/c. At midrapidity, epos and qgsjet-ii predict larger per-event multiplicity probabilities at very low (N ch < 3) and very high (N ch > 100) particle multiplicities, whereas pythia 6 and 8 feature higher yields in the intermediate region N ch ≈ 30-80. These results provide useful information for the estimation of the detector occupancies and energy deposits from pileup collisions at the expected large FCC-hh/SppC luminosities.

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Transverse-momentum distributions of charged particles produced inp¯pinteractions at √s¯=630 and 1800 GeV

Cited by 196 publications

References 19 publications

Scaling Properties of the Mean Multiplicity and Pseudorapidity Density in e−+e+, e±+p, p( p ¯ )+p, p+A and A+A(B) Collisions

Scaling Properties of the Mean Multiplicity and Pseudorapidity Density in e−+e+, e±+p, p( p ¯ )+p, p+A and A+A(B) Collisions

Transverse-momentum and pseudorapidity distributions of charged hadrons in pp collisions at $\sqrt{s} = 0.9 $ and 2.36 TeV

Global properties of proton-proton collisions at s = 100 $$ \sqrt{\mathrm{s}}=100 $$ TeV

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