A METHOD FOR THE CALCULATION OF ELECTRON ENERGY-STRAGGLING SPECTRA

Citation
J. Mclellan et al., A METHOD FOR THE CALCULATION OF ELECTRON ENERGY-STRAGGLING SPECTRA, Medical physics, 21(3), 1994, pp. 367-378
Citations number
42
Categorie Soggetti
Radiology,Nuclear Medicine & Medical Imaging
Journal title
ISSN journal
00942405
Volume
21
Issue
3
Year of publication
1994
Pages
367 - 378
Database
ISI
SICI code
0094-2405(1994)21:3<367:AMFTCO>2.0.ZU;2-D
Abstract
To calculate electron beam dose distributions accurately, numerical me thods of electron transport calculations must account for the statisti cal variation (or ''straggling'') in electron energy loss. This paper shows that the various energy straggling theories that are applicable to short path lengths all derive from a single statistical model, know n as the compound Poisson process. This model in tum relies on three a ssumptions: (1) the number of energy-loss events in a given path lengt h is Poisson distributed; (2) events are mutually independent; and (3) each event has the same probability distribution for energy loss (i.e ., the same energy-loss cross section). Applying the principles of the compound Poisson process and using fast Fourier transforms, a new met hod for calculating energy-loss spectra is developed. The spectra calc ulated using this method for 10, 20, and 30 MeV electrons incident on graphite and aluminum absorbers agreed with Monte Carlo simulations (E Gs4) within 1% in the spectral peak. Also, stopping powers derived fro m the calculated spectra agreed within 1.2%, with stopping powers tabu lated by the International Commission on Radiation Units and Measureme nts. Several numerical transport methods ''propagate'' the electron di stribution (in position, direction, and energy) over small discrete in crements of path length. Thus the propagation of our calculated spectr a over multiple path length increments is investigated. For a low atom ic number absorber (graphite in this case), calculated spectra agreed with EGS4 Monte Carlo simulations over the full electron range, provid ed the path length increments were sufficiently small (less than 0.5 g /cm2). It is concluded from these results that numerical methods of el ectron transport should restrict the size of path length increments to less than 0.5 g/cm2 if energy straggling is to be modeled accurately.