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Geant4 Collaboration Meeting REVERSE MONTE CARLO – STATUS, PERSPECTIVE
Giovanni Santin, ESA/ESTEC Laurent Desorgher, CHUV Fermilab 28 September - 3 October 2015
REVERSE MONTE CARLO STATUS, PERSPECTIVE Giovanni Santin, - - PowerPoint PPT Presentation
Geant4 Collaboration Meeting REVERSE MONTE CARLO STATUS, PERSPECTIVE Giovanni Santin, ESA/ESTEC Laurent Desorgher, CHUV Fermilab 28 September - 3 October 2015 Overview Recap of Reverse / Adjoint Monte Carlo in Geant4 Slides
Giovanni Santin, ESA/ESTEC Laurent Desorgher, CHUV Fermilab 28 September - 3 October 2015
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1. Simulation starts at new “adjoint source” close to target and scores at external source
2. Check at external source, the adjoint particle must belong to the real source phase-space, otherwise it is rejected 3. Each adjoint physics process modifies particle weight 4. Final weight at external source determines probability
5. This weight is used as source biasing for a forward/direct simulations, from the adjoint source towards the target
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in the 1960’s
in NOVICE was available to space community. It soon became an indispensable tool, a de facto standard particularly in the industrial context.
capabilities available in MCNP, AMC, ITS 5.0
in GEANT4 (e-, 𝜹, protons, ions) and FASTRAD (e-, 𝜹) - two separate development lines funded by ESA and CNES
Giovanni Santin - Geant4 Collaboration Workshop 2015
5 T M Jordan, IEEE Trans Nucl Sci., 23, p1857, 1976 P . Pourrouquet et al., NSREC 2011 Conference Proceedings
distributed in the G4 toolkit (ESA funded)
application developer – Geant4 example extended/biasing/ReverseMC1 – Publication in NIMA:
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– Ionisation (continuous and discrete) for e-, proton and ion – Multiple scattering – Bremsstrahlung – Compton scattering – Photo-electric effect
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Tantalum plates 0.5mm thick Spherical Al shielding radius 10 cm user defined thickness Energy deposited in small Si sensitive cylinder with variable size External spherical source radius 10 cm primary particles e- , and proton
toolkit classes
(e.g. exp-E/E0, E-α, arb.) – Computation of response matrix/yield function
– Automatic stop when user-defined precision is reached
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volume (== RMC source volume)
convergence
gamma interactions / high reverse weight? – Attempt to limit impact with splitting
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fast and gamma spectra look reasonably correct (w.r.t Geant4 Forward MC)
significant peaks and slow convergence
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faster without reverse Photo-Electric and reverse Compton
appear as important for final dose end-points
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development, although now in new environment at CHUV Lausanne
– Reliable Reverse MC would be of interest for industry and research institutes for all missions, from Science to Earth Observation to Telecomm
application (GRAS in this case) – Systematic testing and fresh look at code being organised – Design changes required to move to MT – Very specific expertise in RMC and biasing is required, nevertheless ideas and practical help appreciated
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Thank you
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