1989
DOI: 10.1088/0954-3899/15/6/018
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A Monte Carlo generator for cosmic-ray collisions

Abstract: A MC generator incorporating the new features of hadronic multiproduction, observed at the CERN collider with the European hybrid spectrometer, has been developed using considerations based on the dual parton model. This semi-empirical model is especially efficient at reproducing the complex characteristics of semi-inclusive data under the principle of scaling in the central region for relative rapidity density against z, and violation of KNO scaling. Extended to include p-A collisions, such as a triple-Gaussi… Show more

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Cited by 70 publications
(56 citation statements)
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“…Inelastic proton-air cross sections as a function of energy, according to experimental data (Mielke et al, 1994;Yodh et al, 1983;Gaisser, et al, 1987;Baltrusaitis et al, 1984;Honda et al, 1993;Aglietta et al, 1997) and according to the models in the CORSIKA and MOCCA Monte Carlo Programs. VENUS (Werner, 1993), HDPM (Capdevielle, 1989) and DPMJET (Ranft, 1995) are the hadronic interaction models at high energies provided in the CORSIKA Monte Carlo Program. From Knapp, 1997.…”
Section: Longitudinal Development Of Proton Iron and Gamma-ray Primmentioning
confidence: 99%
“…Inelastic proton-air cross sections as a function of energy, according to experimental data (Mielke et al, 1994;Yodh et al, 1983;Gaisser, et al, 1987;Baltrusaitis et al, 1984;Honda et al, 1993;Aglietta et al, 1997) and according to the models in the CORSIKA and MOCCA Monte Carlo Programs. VENUS (Werner, 1993), HDPM (Capdevielle, 1989) and DPMJET (Ranft, 1995) are the hadronic interaction models at high energies provided in the CORSIKA Monte Carlo Program. From Knapp, 1997.…”
Section: Longitudinal Development Of Proton Iron and Gamma-ray Primmentioning
confidence: 99%
“…QGSJet 01 [16,17] and Sibyll 2.1 [18,19]. Furthermore it must be kept in mind that many other models are considered as outdated or just not fashionable like neXus [20,21], HDMP [22], DPMJET [23], DTUJET [24], VENUS [25] etc. .…”
Section: Introductionmentioning
confidence: 99%
“…2a for the relation 3 − 1 with √ s = 8 TeV included in GHOST. The procedure is the same than the generation introduced in CORSIKA [2]. For each random value of N ch one complete set of rapidities is generated by GHOST for all secondaries (as indicated is subsection 3 − 3).…”
Section: Pseudorapidity Distribution and Mean Multiplicitymentioning
confidence: 99%
“…Section 3 is focused on the new four component model GHOST (Generator Hadronic Oversteering Secondary Treatment) [1] used to explore the fluctuations of multiplicity and the violation of KNO (Koba-Nielsen-Olsen) scaling. The extension of the generator HDPM [2] previously inserted in CORSIKA [3] is described in [1]. Section 4 recalls a few measurements not explained in cosmic ray data above √ s = 5 TeV, especially in the case of very high energy spectra of secondaries measured in EAS and γ-ray families.…”
Section: Introductionmentioning
confidence: 99%