Geant4 developments and applications

By J. Allison, K. Amako, J. Apostolakis, H. Araújo, P. A. Dubois, M. Asai, G. Barrand, R. Capra, S. Chauvie, R. Chytracek and 63 more. IEEE Transactions on Nuclear Science, 2006

6,891 citations recorded by the source corpus.

Subfields: Nuclear and High Energy Physics, Pulmonary and Respiratory Medicine

View Paper: https://www.semanticscholar.org/paper/7ae4141002736bfa7fbb8e74ce0868cacaad8a4c

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Citations in the corpus

Search for dark matter, extra dimensions, and unparticles in monojet events in proton–proton collisions at s=8 TeV (2015, methodology): “All the generated signal and background events are passed through a Geant4 [48,49] simulation of the CMS detector and reconstructed with the same algorithms as used for collision data.”
MaGe-a Geant4-Based Monte Carlo Application Framework for Low-Background Germanium Experiments (2010, background): “M AGE (MAjorana-GErda) is a GEANT4-based [1], [2]”
Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at sqrt(s) = 7 TeV (2011, methodology): “51 [33] GEANT4 Collaboration, “GEANT4: a simulation toolkit”, Nucl.”
Measurement of the Inelastic Proton-Proton Cross Section at root s=13 TeV with the ATLAS Detector at the LHC (2016, methodology): “The detector response is modeled using a simulation based on G eant 4 [19–21].”
Angular analysis and differential branching fraction of the decay $B^0_s\toφμ^+μ^-$ (2015, methodology): “The interaction of the generated particles with the detector, and its response, are implemented using the Geant4 toolkit [21, 22] as described in ref.”
PENELOPE-2006: A Code System for Monte Carlo Simulation of Electron and Photon Transport (2009, neutral): “…et al., 1985), GEANT3 (Brun et al., 1986), EGSnrc (Kawrakow and Rogers, 2001), MCNP (X-5 Monte Carlo Team, 2003), GEANT4 (Agostinelli et al., 2003; Allison et al., 2006), FLUKA (Ferrari et al., 2005), EGS5 (Hirayama et al., 2005), …] have recourse to multiple-scattering theories which allow the…”
Combined fit of spectrum and composition data as measured by the Pierre Auger Observatory (2016, methodology): “As for photodisintegration, here we use the cross sections from [50, 51] (PSB), [61] (TALYS, as described in [49]), and Geant4 [63] total cross sections with TALYS branching ratios ([49]).”
First observation of the decay Bs0 → KS0K∗(892)0 at LHCb (2015, methodology): “The interaction of the generated particles with the detector, and its response, are implemented using the Geant4 toolkit [23] as described in Ref.”
The Majorana Demonstrator Neutrinoless Double-Beta Decay Experiment (2012, methodology): “This suite is run every time there is a major update to MaGe or Geant4 to verify that the critical physics processes are not altered between versions.”
Applications and usage of the real-time Neutron Monitor Database (2011, methodology): “(i) CR trajectories through geomagnetosphere will be calculated with the Geant4 software (Allison et al., 2006) MAGNETOCOSMICS (http://cosray.”
Search for CP violation in $D^{\pm}\rightarrow K^0_{\mathrm{S}} K^{\pm}$ and $D^{\pm}_{s}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}$ decays (2014, methodology): “bed by EvtGen [23], in which nal state radiation is generated using Photos [24]. The interaction of the generated particles with the detector and its response are implemented using the Geant4 toolkit [25] as described in Ref. [26]. 3 Candidate selection Candidate D (s) !K 0 S h and D (s) !˚ˇ decays ”
The P2 experiment (2018, methodology): “resolution tracking also allows for the study of backgrounds and position and momentum dependent systematic eects. The tracking detector geometry and reconstruction was developed using a full Geant4 [62,63,64] based simulation of the P2 setup including a detailed eld map based on the FOPI solenoid m”