I: SRSMC vs Film
As previously discussed, due to the composition of the bespoke head and neck phantom plan verifications were historically exposed on film in the transverse plane. Initial commissioning of the SRSMC was done with a coplanar set up meaning in the coronal plane, therefore it was not possible to have the diode and film exposures in the same plane for direct comparison.
Instead, for commissioning, we verified that pass rates were of a similar magnitude for the plan as a whole complex treatment, i.e. pass rates > 95% at 1%2mm gamma index would have similar pass rates in both the coronal and transverse planes, but would not expect them to be identical.
Average pass rates for a selection (N = 20) of original treatment plans were 91.05% at 3%1mm and 97.29% at 5%1mm. The corresponding average pass rates of the same plans exposed at coplanar angles, on the SRSMC in the coronal plane were 99.41% and 99.9% for 3%1mm and 5%1mm respectively. A selection of these plans covering a range of PTV equivalent diameters are highlighted in Table 1 and average results over all plans summarised in Table 3.
Table 1
Original film plans in transverse plane Vs SRSMC at coplanar and non-coplanar couch angles in coronal plane.
PTV EQD (cm)
|
Film
|
SRSMC
|
Coplanar
|
Non Coplanar
|
3%/1mm
|
5%/1mm
|
3%/1mm
|
5%/1mm
|
3%/1mm
|
5%/1mm
|
1.2
|
97.28
|
98.41
|
97.7
|
100
|
99.3
|
100
|
1.4
|
83.18
|
96.08
|
99.6
|
100
|
100
|
100
|
1.5
|
94.39
|
98
|
100
|
100
|
100
|
100
|
2.4
|
94.06
|
95.94
|
99.6
|
100
|
94.7
|
99.2
|
2.5
|
91.41
|
97.91
|
99.5
|
100
|
99.8
|
100
|
2.6
|
91.81
|
96.96
|
100
|
100
|
99.7
|
100
|
3.4
|
99.16
|
99.71
|
98.6
|
99.8
|
98.8
|
100
|
4.3
|
91.73
|
99.26
|
99.6
|
100
|
100
|
100
|
Differences in pass rates are possibly due to a number of reasons:
-
The original plans were conducted by several different Physicists over a period of a couple of years, meaning inherent variations in output on the day, localisation and user analysis are taken in to account over time, as opposed to the plans for this study which were conducted in single sessions, by a single Physicist.
-
The resolution of the film vs the resolution of the SRSMC diode plane, whereby a higher resolution (film) is more likely to highlight smaller errors, which may not be picked up by the diodes leading to a lower gamma index pass rate.
-
Differences in matching techniques due to the phantoms used. Both methods used CBCT pre-exposure image matching, however the homogenous SRSMC and StereoPHAN phantom has ball bearings embedded for localisation, along with other easily discernible physical features on the CBCT image. 6dof couch corrections were also available, which would not have been present for some of our previous film measurements.
The SRSMC allows exposure in the coronal or sagittal planes, and in order to have a like-for-like comparison, a selection of historic plans were re-exposed using the film holder in the StereoPHAN, then compared to measurements on the SRSMC in the same plane, the results of which are presented in Table 2 and Table 3.
Pass rates for the SRSMC were consistently higher than those obtained with film, being 100% pass rate at 3% 1mm consistently. Differences between film and SRSMC pass rates varied, 0.16–9.37% difference at 3%/1mmv(after re-measurement and verification). The possible reasons for these differences are discussed above. We would not consider the SRSMC results to be a false positive, however when using the device for plan verification users should be aware of these points when replacing film.
Table 2
Direct comparison of film measurements and SRSMC in coronal plane in StereoPHAN phantom.
PTV Eq Di (cm)
|
Film
|
SRSMC
|
Difference
|
3%/1mm
|
5%/1mm
|
3%/1mm
|
5%/1mm
|
3%/1mm
|
5%/1mm
|
1.2
|
97.57
|
98.7
|
100
|
100
|
2.13
|
1.30
|
1.6
|
99.84
|
100
|
100
|
100
|
0.16
|
0.00
|
1.8
|
97.97
|
99.5
|
100
|
100
|
2.03
|
0.50
|
1.9
|
93.88
|
95.5
|
100
|
100
|
6.12
|
4.50
|
2.1
|
99.69
|
99.91
|
100
|
100
|
0.31
|
0.09
|
2.2
|
96.5
|
99.2
|
100
|
100
|
3.50
|
0.80
|
3.0
|
91.92
|
92.31
|
100
|
100
|
8.08
|
7.69
|
3.2
|
99.51
|
97.84
|
100
|
100
|
0.49
|
2.16
|
4.1
|
90.63
|
92.09
|
100
|
100
|
9.37
|
7.91
|
Table 3
Summary of average results for film analysis vs SRSMC in various setups
SRSMC Coplanar
|
SRSMC Non-Coplanar
|
Film: Custom Phantom
|
Film: StereoPHAN
|
3%/1mm
|
5%/1mm
|
3%/1mm
|
5%/1mm
|
3%/1mm
|
5%/1mm
|
3%/1mm
|
5%/1mm
|
99.3
|
100
|
99.41
|
99.9
|
91.05
|
97.29
|
96.39
|
97.23
|
II: CAX Diode vs Ionisation Chamber:
Measurement on the SRSMC at non-coplanar geometry allows direct comparison of the cumulative dose measured on the CAX Diode and with an ionisation chamber at the same position. Results showed good agreement between the ion chamber measurement and the central diode. It was noted that the results for the chamber are from historic measurements and retrospectively compared to recent CAX measurements done as part of this study. Similar issues as those discussed above, with different team members taking measurements and inherent daily machine variations were taken into consideration when interpreting the differences between the ion chamber and CAX diode, summarised as a selection of plans in Table 4 and average of all plans in Table 5.
The large discrepancy of 3.47% was attributed to a small volume PTV (1.2cm equivalent diameter). This also corresponded to -4.43% difference seen in the CAX1 (measured) vs CAX2 (TPS) measurement. However, in this instance, the actual difference in diode vs ion chamber was 0.34%. Although this was a large discrepancy for both the difference in diode and chamber measurement when compared to the TPS, the diode accurately reflects what is measured by the chamber, therefore we were satisfied that the CAX diode is a suitable surrogate for an ion-chamber to measure point dose.
Table 4
Selection of Ion Chamber and CAX Diode measurements. (* Highlighted and discussed result)
PTV Equivalent Diameter (cm)
|
IC Vs TPS
|
CAX Diode Vs IC
|
CAX1 Vs CAX 2
|
1.2*
|
3.47
|
-0.34
|
-4.43
|
1.4
|
0.66
|
-2.22
|
1.36
|
1.4
|
1.06
|
-1.69
|
-1.68
|
1.5
|
3.39
|
-1.85
|
-1.87
|
1.8
|
1.88
|
0.66
|
-1.74
|
2.1
|
-0.38
|
-1.09
|
-2.67
|
2.4
|
1.21
|
0.62
|
-3.84
|
2.5
|
-0.48
|
-2.22
|
-0.48
|
3.4
|
1.47
|
-0.55
|
-3.85
|
4.3
|
2.57
|
-2.14
|
0.08
|
Table 5
Summary of Ion Chamber and CAX Dose Measurements.
Variables
|
Mean Difference (%)
|
Standard Deviation
|
Range of Differences (%)
|
Ion Chamber TPS Dose vs Exposed Dose
|
0.72
|
1.5
|
-2.49 to 3.47
|
Ion Chamber vs CAX Diode Dose
|
-0.48
|
1.35
|
-2.57 to 0.84
|
CAX 1 vs CAX 2 Dose
|
-0.91
|
1.51
|
-4.43 to 1.92
|
III: 6FFF vs 6WFF.
Exposures used at commissioning of 6FFF (N = 10) were utilised here to investigate the SRSMC gamma pass rates when the same plan is exposed with and without a flattening filter. The differences in pass rates were negligible, and the average gamma analysis pass rates and differences are presented in Table 6.
Table 6
Summary of average gamma pass rates and average differences for treatments using 6WFF and 6FFF
|
6WFF
|
6FFF
|
Difference (%)
|
|
3% 1mm
|
5% 1mm
|
3% 1mm
|
5% 1mm
|
3% 1mm
|
5% 1mm
|
Ave
|
99.4
|
100.0
|
99.0
|
99.9
|
0.4
|
0.1
|
SD
|
1.0
|
0.1
|
1.0
|
0.3
|
1.3
|
0.3
|
Min
|
96.9
|
99.7
|
97.2
|
98.9
|
-2.3
|
-0.3
|
Max
|
100.0
|
100.0
|
100.0
|
100.0
|
2.8
|
1.1
|
IV: Co-planar vs non-coplanar.
A different cohort of clinical plans used for commissioning initially exposed with all fields to be coplanar were repeated using couch angles determined by HA planning techniques (N = 20). Plans analysed were selected to cover all PTV sizes and non-coplanar angles. The average of the pass rates for coplanar and non-coplanar are summarised in Table 7.
Table 7
Summary of average pass rates for the same plans done at coplanar and non-coplanar angles
Coplanar
|
Non-Coplanar
|
3% 1mm
|
5% 1mm
|
3% 1mm
|
5% 1mm
|
99.28
|
99.95
|
99.41
|
99.90
|
No significant difference in results were noted when the same plan is exposed at couch 0 and when the couch is rotated.
V: Isocentric vs Off-axis
A retrospective review and comparison of the pass rates of plans done at isocentric set up and off axis covering all target sizes and lateral shifts were compared. A selection are presented in Table 8, and summarised in Table 9.
Table 8
Pass rates for selection of plans at both Isocentric and off axis locations.
|
PTV Eq Di (cm)
|
3% 1mm
|
5% 1mm
|
Isocentric
|
1.2
|
99.7
|
100
|
2.1
|
100
|
100
|
2.6
|
99.9
|
100
|
3.0
|
100
|
100
|
4.4
|
100
|
100
|
Off-Axis
|
1.3
|
96.1
|
97.7
|
1.4
|
99.3
|
100
|
1.6
|
99.3
|
99.9
|
2.2
|
98.1
|
100
|
2.6
|
100
|
100
|
Table 9
Summary of average pass rates for isocentric and off-axis plans
Iso
|
Off Axis
|
3% 1mm
|
5% 1mm
|
3% 1mm
|
5% 1mm
|
99.58
|
100.00
|
97.86
|
99.66
|
As both sets of results give a clinical pass, the slight difference in results was deemed to be of no concern. The 3% 1mm off-axis results tended to have a lower passing rate when exposed at non-coplanar angles, likely due to inclusion of lateral couch movements introducing uncertainties which are reflected in the final measurement. However, these were still comfortably within the acceptable limits and tolerances, but the lower pass rate fortifies the need for an isocenter verification test, such as the Winston-Lutz test, to be carried out routinely as part of a SRT program. At WRCC this is checked weekly.