Skip to main page content
U.S. flag

An official website of the United States government

Dot gov

The .gov means it’s official.
Federal government websites often end in .gov or .mil. Before sharing sensitive information, make sure you’re on a federal government site.

Https

The site is secure.
The https:// ensures that you are connecting to the official website and that any information you provide is encrypted and transmitted securely.

Access keys NCBI Homepage MyNCBI Homepage Main Content Main Navigation
. 2019 Jul-Sep;44(3):145-155.
doi: 10.4103/jmp.JMP_17_19.

An Experimental Slope Method for a More Accurate Measurement of Relative Radiation Doses using Radiographic and Radiochromic Films and Its Application to Megavoltage Small-Field Dosimetry

Affiliations

An Experimental Slope Method for a More Accurate Measurement of Relative Radiation Doses using Radiographic and Radiochromic Films and Its Application to Megavoltage Small-Field Dosimetry

Raghavendra Holla et al. J Med Phys. 2019 Jul-Sep.

Abstract

Purpose: An experimental method using the linear portion of the relative film dose-response curve for radiographic and radiochromic films is presented, which can be used to determine the relative depth doses in a variety of very small, medium, and large radiation fields and relative output factors (ROFs) for small fields.

Materials and methods: The film slope (FS) method was successfully applied to obtain the percentage depth doses (PDDs) for external beams of photon and electrons from a Synergy linear accelerator (Elekta AB, Stockholm, Sweden) under reference conditions of 10 cm × 10 cm for photon beam and nominal 10 cm × 10 cm size applicator for electron beam. For small-field dosimetry, the FS method was applied to EDR2 films (Carestream Health, Rochester, NY) for 6 MV photon beam from a linac (Elekta AB, Stockholm, Sweden) and small, circular radiosurgery cones (Elekta AB, Stockholm, Sweden) with diameters of 5, 7.5, 10, 12.5, and 15 mm. The ROFs for all these cones and central axis PDDs for 5, 10, and 15 mm diameter cones were determined at source-to-surface distance of 100 cm. The ROFs for small fields of CyberKnife system were determined using this technique with Gafchromic EBT3 film (Ashland, NJ, USA). The PDDs and ROFs were compared with ion chamber (IC) and Monte Carlo (MC) simulated values.

Results: The maximum percentage deviation of PDDFS with PDDIC for 4, 6, and 15 MV photon beams was within 1.9%, 2.5%, and 1.4%, respectively, up to 20-cm depth. The maximum percentage deviation of PDDFS with PDDIC for electron beams was within 3% for energy range studied of 8-15 MeV. The gamma passing rates of PDDFS with PDDIC were above 96.5% with maximum gamma value of >2, occurring at the zero depths for 4, 6, and 15 MV photons. For electron beams, the gamma passing rates between PDDFS with PDDIC were above 97.7% with a maximum gamma value of 0.9, 1.3, and 0.7 occurring at the zero depth for 8, 12, and 15 MeV. For small field of 5-mm cone, the ROFFS was 0.665 ± 0.021 as compared to 0.674 by MC method. The maximum percentage deviation between PDDFS and PDDMC was 3% for 5 mm and 10 mm and 2% for 15 mm cones with 1D gamma passing rates, respectively, of 95.5%, 96%, and 98%. For CyberKnife system, the ROFFS using EBT3 film and MC published values agrees within 0.2% for for 5 mm cone.

Conclusions: The authors have developed a novel and more accurate method for the relative dosimetry of photon and electron beams. This offers a unique method to determine PDD and ROF with a high spatial resolution in fields of steep dose gradient, especially in small fields.

Keywords: CyberKnife; EBT3 film; EDR2 film; Percentage depth dose; film slope method; relative dosimetry; relative output factor; small-field dosimetry.

PubMed Disclaimer

Conflict of interest statement

There are no conflicts of interest.

Figures

Figure 1
Figure 1
(a) and (b) Phantom measurement of PDD at points A and B at depths ‘dmax’ and ‘d’ with dose rates ‘Dmax’ and ‘Dd’, respectively
Figure 2
Figure 2
The different representations of characteristic curves used in dosimetry for EDR2 Ready-Pack film using (a) net optical density versus Log10 (dose) or (b) net optical density versus dose for 6 MV photon beam
Figure 3
Figure 3
Hurter and Driffield curve using Gafchromic EBT3 film for 6 and 15 MV photon beams showing the energy dependence
Figure 4
Figure 4
The linear portion of the relative film dose–response plots at two different depths A and B with the slopes, mA and mB
Figure 5
Figure 5
The relative film dose response at their respective depths for determining percentage depth dose; (a) EDR2 Ready-Pack films, (b) Gafchromic EBT3 films, Photon energy: 6 MV photon, field size: 10 cm × 10 cm, source-to-surface distance: 100 cm
Figure 6
Figure 6
The relative film dose response at their respective linear ranges plotted at various depths using EDR2 Ready-Pack film to determine percentage depth dose of 6 MV photon beam with (a) 5-mm and (b) 10-mm diameter stereotactic radiosurgery cones
Figure 7
Figure 7
Calculated slopes from the linear curve fit of the relative film dose–response curves for radiosurgery fields of 5, 7.5, 10, 12.5, and 15 mm diameter at ‘dmax’ using EDR2 film. The output factors for these circular fields were calculated by normalizing the slopes from the linear portion of the relative film dose–response curve to the slope of reference field, 10 cm × 10 cm
Figure 8
Figure 8
Percentage depth dose comparison for different energy beams; using EDR2 film; (a) 6 MV photon, (b) 4 MV photon, (c) 15 MV photon, (d) 8 MeV electron, (e) 12 MeV electron, and (f) 15 MeV electron; using EBT3 film (g) 6 MV photon; percentage depth dose: Film slope method (dotted black line), PTW 31010 (solid red line); 1D gamma evaluation between film slope method and PTW 31010 (solid orange line)
Figure 9
Figure 9
Percentage depth dose comparison for different radiosurgery cones. (a) 5 mm diameter, (b) 10 mm diameter, and (c) 15 mm diameter; percentage depth dose: Film slope method (dotted black line), Monte Carlo (solid red line), diode (N60008) (solid blue line), and 1D gamma evaluation between film slope method and Monte Carlo (solid orange line). Percentage depth dose in the buildup region for (d) 5 mm diameter, (e) 10 mm diameter, and (f) 15 mm diameter

Similar articles

References

    1. International Atomic Energy Agency. Absorbed dose Determination in External Beam Radiotherapy: An International Code of Practice for Dosimetry Based on Standards of Absorbed dose to Water. Vienna, Austria: Technical Reports Series; 2000. p. 398.
    1. A protocol for the determination of absorbed dose from high-energy photon and electron beams. Med Phys. 1983;10:741–71. - PubMed
    1. Almond PR, Biggs PJ, Coursey BM, Hanson WF, Huq MS, Nath R, et al. AAPM's TG-51 protocol for clinical reference dosimetry of high-energy photon and electron beams. Med Phys. 1999;26:1847–70. - PubMed
    1. Scott AJ, Nahum AE, Fenwick JD. Using a Monte Carlo model to predict dosimetric properties of small radiotherapy photon fields. Med Phys. 2008;35:4671–84. - PubMed
    1. Palmans H, Andreo P, Huq MS, Seuntjens J, Christaki K. Technical Report Series No 483. Vienna: International Atomic Energy Agency; 2017. [Last accessed on :2019 May 17]. Dosimetry of Small Static Fields used in External Beam Radiotherapy: An IAEA-AAPM International Code of Practice for Reference and Relative dose Determination. Available from: http://www-pub.iaea.org/books/IAEABooks/11075/Dosimetry-of-Small-Static-... .