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Megavoltage Linac Photons

Radiotherapy calibrations index:

Radiotherapy ionisation chambers can now be calibrated directly in megavoltage photon beams from a medical linear accelerator

The accelerator (Figure 1) and the beams used for the calibration are specified in Table 1.

Table 1: Megavoltage photon beams available for calibration at ARPANSA

Beam1 TPR20,10 Rate2 Pulse rate
6 MV 0.673 400 MU/min 400 Hz
10 MV 0.734 375 MU/min 200 Hz
18 MV 0.777 490 MU/min 200 Hz

1 Nominal accelerating potential
2Linac output rate. The linac delivers approximately 1 cGy/MU at dmax in an isocentric setup (100 cm source-detector distance) with a 10 cm x 10 cm field.

The Elekta Synergy Linac at ARPANSAFigure 1: The Elekta Synergy Linac at ARPANSA

Advantages

The direct megavoltage calibration service is intended to complement the 60Co calibration service. Instead of using kQ correction factors calculated from the nominal dimensions of the chamber, the direct calibration allows these factors to be measured and interpolated to the user’s beam qualities.

The direct calibration is slightly more accurate than using 60Co and does not rely on assumptions about the behaviour of the ionisation chamber. A discussion of the implications of the new services is available in reference [2].

Validation

ARPANSA staff prepare a monitor chamber (left) used to confirm the linac output before measurements with the primary standard graphite calorimeter (right)Figure 2: ARPANSA staff prepare a monitor chamber (left) used to confirm the linac output before measurements with the primary standard graphite calorimeter (right)

The technical details of the work done to implement the primary standard of absorbed dose on a linear accelerator are described in a recent Technical Report, TR166 [1]. The results of international comparisons of absorbed dose to water for linac beams performed in 2012 and 2013 are available in publications [3] and [4].

Extract from the linac photon calibration report

The linac megavoltage photons are measured in addition to 60Co, and the results are presented as shown in Figure 3 as ratios to the chamber calibration coefficient at 60Co. To enable users to be able to interpolate these results to different beam qualities, a quadratic fit is also given the report. An example is shown in Figure 4.

Excerpt from a calibration certificate for a Farmer-type chamber. To find kQ for a user beam, a simple quadratic equation is usedFigure 3: Excerpt from a calibration certificate for a Farmer-type chamber. To find kQ for
a user beam, a simple quadratic equation is used.

 

Example calibration results. The calibration coefficient ND,w is given for 60Co. The linear accelerator calibration results are presented as correction factors for the different beamsFigure 4: Example calibration results. The calibration coefficient ND,w is given for 60Co. The linear accelerator calibration results are presented as correction factors for the different beams

References

[1]. The Australian Primary Standard for absorbed dose to water (graphite calorimeter), Ganesan Ramanathan, Peter Harty, Tracy Wright, Jessica Lye, Duncan Butler, David Webb and Robert Huntley, ARPANSA Technical Report Series No. 166. Published June 2014. Available online at: TR-166.
[2] Direct megavoltage photon calibration service in Australia, D. J. Butler, G. Ramanathan, C. Oliver, A. Cole, J. Lye, and P.D. Harty, T. Wright, D. V. Webb, Australas. Phys. Eng. Sci. Med. (2014) Epub ahead of print 22 Aug 2014.
[3] Key comparison BIPM.RI(I)-K6 of the standards for absorbed dose to water of the ARPANSA, Australia and the BIPM in accelerator photon beams, S. Picard, D. T. Burns, P. Roger, P. D. Harty, G. Ramanathan, J. E. Lye, T. Wright, D. J. Butler, A. Cole, C. Oliver, D. V. Webb, Metrologia 2014 51 Tech. Suppl. 06006
[4] Comparison of the NMIJ and the ARPANSA standards for absorbed dose to water in high-energy photon beams, M. Shimizu; Y. Morishita; M. Kato; T. Tanaka; T. Kurosawa; N. Takata; N. Saito; G. Ramanathan; P. D. Harty; C. Oliver; T. Wright; D. J. Butler, Radiation Protection Dosimetry 2014; doi: 10.1093/rpd/ncu272

 

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