2005
DOI: 10.1070/rd2005v010n03abeh000315
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Cited by 62 publications
(55 citation statements)
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“…The Monte Carlo simulation of the beam line and detectors is based on GEANT3 [20] and the hadron production yields from the target are calculated by FLUKA [21]. The calculated neutrino flux is adjusted to agree with the ND ν µ -CC data [17].…”
mentioning
confidence: 99%
“…The Monte Carlo simulation of the beam line and detectors is based on GEANT3 [20] and the hadron production yields from the target are calculated by FLUKA [21]. The calculated neutrino flux is adjusted to agree with the ND ν µ -CC data [17].…”
mentioning
confidence: 99%
“…The air showers have been generated with zenith angle θ distributed as sin θ cos θ (with θ < 65 • ), according to the projection on a surface detector of a isotropic flux of cosmic rays, and with energy ranging between 10 17 eV and 10 19.5 eV, according to a power law spectrum (spectral index γ = −1) and in intervals of 0.5 in the logarithm of energy. Simulations are performed using QGSJET-II.03 [44], QGSJET-I [45] and Epos-1.99 [46] as hadronic interaction models at high energy and FLUKA [47] at low energy. Moreover, seasonal models of the atmospheric conditions (pressure, temperature and air density) as measured in Malargüe [48] are used in addition to the US standard model [49].…”
Section: Time Dependent Simulations With the Full Monte Carlo Approachmentioning
confidence: 99%
“…To simulate the hadron production yields from the carbon target, FLUKA [52] is used in this analysis. Finally, NEUGEN3 [53] is used in order to simulate neutrino interactions and the re-interactions of the produced hadrons within the nuclei.…”
Section: Monte Carlo and Reconstructionmentioning
confidence: 99%