The impact of ion chamber components on kB,Q for reference dosimetry in MRgRT
Julia Navarro Campos,
The Netherlands
MO-0052
Abstract
The impact of ion chamber components on kB,Q for reference dosimetry in MRgRT
Authors: Julia Navarro Campos1, Jacco de Pooter2, Leon de Prez2
1LUMC, Radiotherapy, Leiden, The Netherlands; 2VSL Dutch Metrology Institute, Ionising radiation, Delft, The Netherlands
Show Affiliations
Hide Affiliations
Purpose or Objective
For reference dosimetry in MRgRT, kB,Q
is used to correct for the impact of the magnetic field on the chamber
calibration coefficient. It has been demonstrated that for accurate simulation
of kB,Q the dead volume (DV) must be considered. This work
goes one step further by analysing the different contribution of all chamber
components to kB,Q.
Material and Methods
Based on the blueprints the Farmer-type chamber
PTW 30013 geometry was modelled in PENELOPE (2014). Two DVs were modelled; one
based on published data (Pojtinger et al, 2019) (DV1) and one
determined using FEM simulations (DV2). Radiation fields (10x10 cm2)
were based on phase space files of a 60Co source and a 7MV MRI-linac.
The model was validated against measurements with a setup using an
electromagnet and a 60Co source (0 – 1.5 T) and an MRI-linac (0 and
1.5 T) (de Prez et al, 2019). Simulations were performed with the PENMAIN
routine with magnetic field routines implemented for both parallel and
perpendicular orientations of the chamber and the magnetic (B) field, and for
several B-field strengths between 0 T and ±1.5 T. To study the dose
contribution to the sensitive volume (SV = cavity – DV) from the electrons
produced in certain components of the chamber (wall, central electrode (CE),
guard, stem, phantom), the labelling of the particles was implemented in
PENMAIN. A separate model with each solid component of the chamber modelled as
liquid water (indicated by PTW 30013 (water)) was used to investigate the
impact of material choice on kB,Q.
Results
The simulated kB,Q results agree
better with the measured kB,Q when the DV is considered. The difference
between measured kB,Q and simulated kB,Q reduces
from at maximum 0.6% for DV1 to 0.4% for DV2 at B = 0.75
T in 60Co. This demonstrates the accuracy of the model, and it shows
that small changes in the DV may have a small impact in the kB,Q.
Figures 1 and 2 show the relative contribution
of each component to the effect of kB,Q (i.e., kB,Q-1).
The negative value in the figure means an increase in the contribution from
that component when the B is present.
Figure 1 demonstrates that the contribution to
the SV dose from the bodies closer to the SV is higher than without B. For
parallel orientation, the guard and the stem have higher impact on the dose to
the SV. For the perpendicular orientation the wall contribution is more
important. For all orientations the CE has a similar increased contribution
Figure 2 shows that the general behaviour of
the contribution to the dose of the different components is similar. Overall, the
impact to the dose in SV is reduced when the material of each component is
modelled as liquid water.
Conclusion
Small components of the chamber impact kB,Q
considerably. Therefore, chamber design and, to a lesser extent, choice of
material affects kB,Q, and an accurate model of the chamber
components and its further validation are important for correct calculations of
kB,Q.