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On the Monte Carlo simulation of electron transport in the sub‐1 keV energy range
Author(s) -
Thomson Rowan M.,
Kawrakow Iwan
Publication year - 2011
Publication title -
medical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.473
H-Index - 180
eISSN - 2473-4209
pISSN - 0094-2405
DOI - 10.1118/1.3608904
Subject(s) - physics , electron , monte carlo method , momentum (technical analysis) , quantum monte carlo , kinetic energy , uncertainty principle , range (aeronautics) , mean free path , computational physics , position (finance) , quantum , statistical physics , quantum mechanics , statistics , materials science , mathematics , finance , economics , composite material
Purpose: The validity of “classic” Monte Carlo (MC) simulations of electron and positron transport at sub‐1 keV energies is investigated in the context of quantum theory. Methods: Quantum theory dictates that uncertainties on the position and energy‐momentum four‐vectors of radiation quanta obey Heisenberg's uncertainty relation; however, these uncertainties are neglected in “classical” MC simulations of radiation transport in which position and momentum are known precisely. Using the quantum uncertainty relation and electron mean free path, the magnitudes of uncertainties on electron position and momentum are calculated for different kinetic energies; a validity bound on the classical simulation of electron transport is derived. Results: In order to satisfy the Heisenberg uncertainty principle, uncertainties of 5% must be assigned to position and momentum for 1 keV electrons in water; at 100 eV, these uncertainties are 17 to 20% and are even larger at lower energies. In gaseous media such as air, these uncertainties are much smaller (less than 1% for electrons with energy 20 eV or greater). Conclusions: The classical Monte Carlo transport treatment is questionable for sub‐1 keV electrons in condensed water as uncertainties on position and momentum must be large (relative to electron momentum and mean free path) to satisfy the quantum uncertainty principle. Simulations which do not account for these uncertainties are not faithful representations of the physical processes, calling into question the results of MC track structure codes simulating sub‐1 keV electron transport. Further, the large difference in the scale at which quantum effects are important in gaseous and condensed media suggests that track structure measurements in gases are not necessarily representative of track structure in condensed materials on a micrometer or a nanometer scale.