Line: 1 to 1 | ||||||||
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| ||||||||

Line: 20 to 20 | ||||||||

where V is the sensor volume, Φ is the fluence, L | ||||||||

Changed: | ||||||||

< < | The Pythia 8 simulation uses the MSTW2008LO PDF with either the A2 [3] or A3 [4] minimum bias tunes. A description of the ATLAS FLUKA simulation framework can be found in [5]. The ATLAS detector geometry models are not identical between Geant 4 and FLUKA - the former uses the full geometry model employed by the standard ATLAS Monte Carlo production system [1] while the latter uses a simplified standalone geometry. The predictions are mirrored for +/- |z|, so there is symmetry by construction. Only Monte Carlo statistical uncertainties are shown for the simulation predictions. Due to the more complex geometry used by Geant 4, the statistical uncertainties are enhanced (from the tilt of the IBL staves in φ); the FLUKA simulation also uses a factor of 5 more events than the Geant4 prediction. | |||||||

> > | The Pythia 8 simulation uses either the A2 minimum bias tune [3], or the A3 tune [4]. A description of the ATLAS FLUKA simulation framework can be found in [5]. The ATLAS detector geometry models are not identical between Geant 4 and FLUKA - the former uses the full geometry model employed by the standard ATLAS Monte Carlo production system [1] while the latter uses a simplified standalone geometry. The predictions are mirrored for +/- |z|, so there is symmetry by construction. Only Monte Carlo statistical uncertainties are shown for the simulation predictions. Due to the more complex geometry used by Geant 4, the statistical uncertainties are enhanced (from the tilt of the IBL staves in φ); the FLUKA simulation also uses a factor of 5 more events than the Geant4 prediction. | |||||||

[0] GEANT4 Collaboration, GEANT4: a simulation toolkit, Nucl. Instrum. Meth. A 506 (2003) 250. |

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