
Figure 1
Photo of the semi-anthropomorphic CIRS Thorax phantom with interchangeable rod inserts (left) and its CT image (right). Positions of 10 interchangeable rod inserts are marked with numbers from 1 to 10. Five measuring points are in the water equivalent part of the phantom (grey area), four points are in the lung density equivalent material (black area), and one point is in the bone density equivalent part of the phantom (white area).
Table 1
Irradiation set-ups for measurements in 6 MV photon beam used for experimental verification of the Monaco ver. 5.11 treatment planning systems (TPS) calculation algorithm in the semi-anthropomorphic CIRS Thorax phantom. Reference and measuring points (I1 to I10) are shown in the last two columns; subscripts 1 to 10 correspond to the labelling in Figure 1
| Set-up | Irradiation geometry | Field size [cm2] | SSD/SAD | Gantry angle [°] | reference point | measuring points |
|---|---|---|---|---|---|---|
| 1 | Single square fields | 10×10 | SSD | 0 | I5 | I1, I3, I5-10 |
| 2 | 10×10 | SAD | 0 | I5 | I, I, I135-10 | |
| 3 | 4×4 | SAD | 0 | I5 | I1-9 | |
| 4 | 10×10 | SAD | 90 | I3 | I2-10 | |
| 5 | Rectangular field | 10× 15 | SAD | 300 | I1 | I1, I4, I6-8, I10 |
| 6 | Single asymmetric fields | (6+8)×15 | SAD | 0 | I5 | I1-10 |
| 7 | (3+8)×15 | SAD | 90 | I5 | I, I15-10 | |
| 8 | (4+10)×15 | SAD | 180 | I5 | I1-3, I5-10 | |
| 9 | (3+7)×15 | SAD | 300 | I5 | I2-10 | |
| 12×10 | SAD | 0 | ||||
| 10 | 4 fields (box) | 12×10 | SAD | 180 | I5 | I2-5 |
| 12×8 | SAD | 90 | ||||
| 12×8 | SAD | 270 | ||||
| 4×4 | SAD | 30 | ||||
| 11 | 3 fields | 16×4 | SAD | 90 | I5 | I2, I5-9 |
| 16×4 | SAD | 270 | ||||
| 12 | Diamond-shaped field | 14×14 | SAD | 0 | I3 | I1, I3, I5-10 |
| 13 | Irregular L shaped field | / | SAD | 45 | I1 | I1-2, I4-6, I8-10 |
| 14 | MLC cylinder shaped field | / | SAD | 0 | I2 | I1,2, I5, I8,9, I10 |
| 16×4 | SAD | 90 | ||||
| 15 | 3 non-coplanar fields | 16×4 | SAD | 270 | I5 | I1, I5-6, I8, I10 |
| 4×4a | SAD | 30 |

Figure 2
CT image of the CIRS Thorax phantom: water equivalent insert inside BDE part of the phantom (A); a BDE insert inside bone density equivalent (BDE) part of the phantom (B) and cross-section of small “water cylinders” of different dimensions delineated inside BDE part of the phantom to find limits for calculating geometry where cavity theory applies (top right).

Figure 3
Mean percentage dose differences and between calculated and measured doses in different parts of the CIRS Thorax phantom (water, lung, and bone density equivalent materials) for both calculation options built in the Monaco TPS: dose-to-medium Dm and dose-to-water Dw. Error bars represent corresponding combined uncertainties.
Table 2
Differences and between two different calculation options in the Monaco ver. 5.11. treatment planning systems (TPS) and measured data obtained in the bone density equivalent (BDE) part of the CIRS Thorax phantom, according to Eqs. [1] and [2]. Two phantom assemblies and three simple beam setups were considered for this part of the study
Table 3
Mean differences, and between calculated and measured doses in the bone density equivalent (BDE) part of the CIRS Thorax phantom for Dm and Dw calculation approaches, respectively. The absorbed doses were calculated using the Monaco ver. 5.11 treatment planning systems (TPS) in the center of delineated “water cylinders” of volume V, in the BDE part of the phantom. Corresponding combined uncertainties are denoted as uc,m and uc,w for dose-to-medium and dose-to-water calculation options, respectively
| V [cm3] | [%] | uc,m[%] | [%] | uc,w[%] |
|---|---|---|---|---|
| 0 | - 3.9 | 2.1 | 4.4 | 1.9 |
| 0.035 | - 2.6 | 1.5 | 2.5 | 1.9 |
| 0.141 | - 1.4 | 1.3 | 1.8 | 1.7 |
| 0.279 | - 0.3 | 1.2 | 1.2 | 1.5 |
| 0.573 | 0.3 | 1.4 | 0.4 | 1.3 |

Figure 4
Average differences and between calculated and measured doses in the bone density equivalent (BDE) part of the CIRS Thorax phantom, as a function of the volumes of the simulated “water cylinders” (see Figure 2 and Table 3). and are presented as individual values/points calculated using Eqs. [1] to, [4], and in the form of two analytical functions from Eqs. [9] and [10]. Error bars represent corresponding uncertainties within 95% confidence limits.