The FLUKA code: Description and benchmarking

By G. Battistoni, F. Cerutti, A. Fassò, A. Ferrari, S. Muraro, J. Ranft, S. Roesler, P. Sala. 2007

1,355 citations recorded by the source corpus.

Subfields: Nuclear and High Energy Physics, Radiation

View Paper: https://www.semanticscholar.org/paper/81a2fac9766faf091dadf55b02fce67a911b7bd0

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Nuclear and High Energy Physics

In Radiation

Citations in the corpus

Experimental Signatures of the Quantum Nature of Radiation Reaction in the Field of an Ultraintense Laser (2017, methodology): “The energy deposited on the scintillator, modeled with FLUKA [35] simulations, is almost linear in the range 10–400 MeV and best fitted (R(2) 1⁄4 95%) by EDEP 1⁄4 2.”
ROOT - A C++ framework for petabyte data storage, statistical analysis and visualization (2009, methodology): “The concrete Monte Carlo implementation (Geant3, Geant4, Fluka) is selected at run time — when processing a ROOT macro where the concrete Monte Carlo object is instantiated.”
The ATLAS Simulation Infrastructure (2010, methodology): “QGSP_BERT_HP—the physics list used for neutron fluence studies and comparisons with the FLUKA simulation package [92, 93].”
A First Baseline for the Magnets in the High Luminosity LHC Insertion Regions (2014, background): “The solution is to have a large aperture triplet, to make space for thick shielding: results from energy deposition simulations [15], [20], [21] show that the magnets can be protected from the collision debris through appropriate shielding.”
The GENIE Neutrino Monte Carlo Generator: Physics and User Manual (2015, background): “kinetic energy larger than 300 MeV and nucleons above 200 MeV), where the mean free path is long compared to the inter-nuclear spacing of roughly 1.8fm and the pion Compton wavelength. Peanut (FLUKA) [112] received a major eﬀort in 1995-9 and is very well adapted to describe processes from 10 MeV to”
The NUMEN project: NUclear Matrix Elements for Neutrinoless double beta decay (2018, methodology): “In order to address the issue quantitatively, a simulation was implemented based on the FLUKA [220] Monte Carlo code.”
THE COSMIC-RAY ENERGY SPECTRUM OBSERVED WITH THE SURFACE DETECTOR OF THE TELESCOPE ARRAY EXPERIMENT (2012, methodology): “…a library of showers generated by the CORSIKA program using QGSJET-II-03 (Ostapchenko 2006) to model high-energy hadronic interactions, FLUKA (Ferrari et al. 2005; Battistoni et al. 2007) to model low-energy hadronic interactions, and EGS4 (Nelson et al. 1985) to model electromagnetic interactions.”
Measurements of neutrino oscillation in appearance and disappearance channels by the T2K experiment with 6.6E20 protons on target (2015, methodology): “We use the FLUKA 2008 package [12,13] to model the interactions of the primary beam protons and the subsequently produced pions and kaons in the graphite target.”
A facility to Search for Hidden Particles (SHiP) at the CERN SPS (2015, methodology): “27: Layout of the facility as implemented in FLUKA [50,51].”
Long-range angular correlations of pi, K and p in p-Pb collisions at root s(NN)=5.02 TeV (2013, methodology): “Therefore, the efﬁciency extracted from GEANT3 was scaled with a factor computed with a dedicated FLUKA [68] simulation as discussed in [64].”
A Proposal for a Three Detector Short-Baseline Neutrino Oscillation Program in the Fermilab Booster Neutrino Beam (2015, methodology): “A FLUKA-based Monte Carlo simulation [68, 69, 124] of the NuMI beam line has been set up according to the available technical drawings [125] for the low energy beam configuration.”