1991
DOI: 10.1007/bf01562339
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Dual parton model with complete formation zone intranuclear cascade for the description of particle production in hadron-nucleus and nucleus-nucleus interactions

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Cited by 56 publications
(54 citation statements)
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“…We use an analytical approximation of the source function based on numerical results using the Monte-Carlo particle interaction code DTUNUC (V2.2) (Möhring & Ranft 1991;Ranft et al 1994;Ferrari et al 1996;Engel et al 1997), which is based on a dual parton model (Capella et al 1994). One has the representation…”
Section: The Evolution Of High Energy Photon Spectramentioning
confidence: 99%
“…We use an analytical approximation of the source function based on numerical results using the Monte-Carlo particle interaction code DTUNUC (V2.2) (Möhring & Ranft 1991;Ranft et al 1994;Ferrari et al 1996;Engel et al 1997), which is based on a dual parton model (Capella et al 1994). One has the representation…”
Section: The Evolution Of High Energy Photon Spectramentioning
confidence: 99%
“…For the calculation of the pion source spectra we use the Monte-Carlo model DTUNUC (V2.2) (Möhring & Ranft 1991;Ranft et al 1994;Ferrari et al 1996a;Engel et al 1997), which is based on a dual parton model (Capella et al 1994). Here we are concerned with high energetic neutrinos resulting from the decays of pions Fig.…”
Section: The Production Of High Energetic Neutrinosmentioning
confidence: 99%
“…In the following we summarize the main ideas of the FZIC model for hadronnucleus and nucleus-nucleus interactions [7,8,9,4,10,11]. The physical picture explaining the absence of the intranuclear cascade at high energies is the concept of the formation zone [19].…”
Section: The Formation Zone Cascade In Target and Projectile Nucleimentioning
confidence: 99%
“…Reinteractions beyond 5 GeV occur much less frequently than reinteractions below 5 GeV and a more detailed treatment would not change the results discussed in this paper. Furthermore, we take into account absorption of low-energy mesons and antiprotons by interactions with two-nucleon systems (for pion absorption we use the cross sections as given by Ritchie [23]) and Pauli's principle [9]. In case no interaction is possible in the considered spectator, we proceed with sampling a cascade step in another spectator.…”
Section: The Formation Zone Cascade In Target and Projectile Nucleimentioning
confidence: 99%