Dt. Burns et al., R(50) AS A BEAM QUALITY SPECIFIER FOR SELECTING STOPPING-POWER RATIOSAND REFERENCE DEPTHS FOR ELECTRON DOSIMETRY, Medical physics, 23(3), 1996, pp. 383-388
For electron beam reference dosimetry in radiotherapy, it is shown tha
t by choosing the reference depth as d(ref)=0.6R(50)-0.1 cm, where R(5
0) is the half-value depth in centimeters, the Spencer-Attix water-to-
air stopping-power ratio at d(ref) is given by ((L) over bar/rho)(air)
(w)=1.2534-0.1487 (R(50))(0.2144). This is derived from data for ((L)
over bar/rho)(air)(w) obtained from realistic Monte Carlo simulations
for 24 clinical beams. The rms deviation of this expression from the M
onte Carlo calculations is 0.16%, with a maximum deviation of 0.26%. T
his approach fully takes into account the spectral differences between
real electron beams of the same R(50) and allows an absorbed-dose cal
ibration at a standards laboratory to be easily and accurately transfe
rred to a reference clinical beam. Using a single parameter to specify
((L) over bar/rho)(air)(w), rather than the two parameters (R(50) and
depth) needed when the reference depth is chosen as the depth of dose
maximum, has the potential to greatly simplify electron beam dosimetr
y protocols and allows the use of a similar formalism for photon and e
lectron beam dosimetry. For use in converting a depth-ionization curve
into a depth-dose curve, a somewhat less accurate but general express
ion for ((L) over bar/rho)(air)(w) as a function of R(50) and depth is
presented.