The contribution from contaminant electrons in the buildup region of a
photon beam must be separated when calculating the close using a phot
on convolution kernel. Their contribution can be extrapolated from fra
ctional depth dose (FDD) data using the fractional depth kerma (or the
''equilibrium dose'') derived from measured quantities such as beam a
ttenuation with depth, phantom scatter factor as a function of field s
ize and depth, and inverse-square law for the incident photon beam. Go
od agreement is observed between the extrapolated and the EGS4 Monte C
arlo simulated, primary dose-to-kerma ratios in the surface region for
the photon beams, excluding electron contamination. The FDD was measu
red using a Scanditronix photon diode and was normalized to a referenc
e depth far beyond maximum range of contaminant electrons. An analysis
for the 8 and 18 MV photon beams from a Varian 2100CD indicates that
at a source-to-surface distance (SSB) of 100 cm, the maximum electron
contaminant dose (relative to its maximum FDD) varies from 1% to 33% f
or 8 MV and 2% to 44% for 18 MV, for square collimator settings rangin
g from 5 to 40 cm (defined at 100 cm from the source). This value at a
depth of maximum dose (2 cm for 8 MV and 3.5 cm for 18 MV) can reach
1% for 8 MV and 2.3% for 18 MV. This contaminant electron dose is almo
st independent of SSD for 8 MV and starts to fall off for 18 MV at SSD
s larger than 120 cm. Compared with the open beam, the contaminant ele
ctron dose increases when a solid tray is used: and the magnitude of i
ncrease increases with field size, reaching 19% and 16% for a 40 x 40
cm(2) field for 8 and 18 MV photons, respectively. The contaminant ele
ctron dose increases slightly for a blocked beam compared with an open
beam of the same field size if a tray is used in both cases. The cont
aminant electron dose for the wedged field is less than that for an op
en field. However, the reduction is less significant at larger collima
tor settings (c = 20 cm) and may increase slightly for 8 MV photons. (
C) 1998 American Association of Physicists in Medicine.