Elsevier

Physica Medica

Volume 30, Issue 1, February 2014, Pages 36-46
Physica Medica

Original paper
High throughput film dosimetry in homogeneous and heterogeneous media for a small animal irradiator

https://doi.org/10.1016/j.ejmp.2013.02.002Get rights and content

Abstract

Purpose

We have established a high-throughput Gafchromic film dosimetry protocol for narrow kilovoltage beams in homogeneous and heterogeneous media for small-animal radiotherapy applications. The kV beam characterization is based on extensive Gafchromic film dosimetry data acquired in homogeneous and heterogeneous media. An empirical model is used for parameterization of depth and off-axis dependence of measured data.

Methods

We have modified previously published methods of film dosimetry to suit the specific tasks of the study. Unlike film protocols used in previous studies, our protocol employs simultaneous multi-channel scanning and analysis of up to nine Gafchromic films per scan. A scanner and background correction were implemented to improve accuracy of the measurements. Measurements were taken in homogeneous and inhomogeneous phantoms at 220 kVp and a field size of 5 × 5 mm2. The results were compared against Monte Carlo simulations.

Results

Dose differences caused by variations in background signal were effectively removed by the corrections applied. Measurements in homogeneous phantoms were used to empirically characterize beam data in homogeneous and heterogeneous media. Film measurements in inhomogeneous phantoms and their empirical parameterization differed by about 2%–3%. The model differed from MC by about 1% (water, lung) to 7% (bone). Good agreement was found for measured and modelled off-axis ratios.

Conclusions

EBT2 films are a valuable tool for characterization of narrow kV beams, though care must be taken to eliminate disturbances caused by varying background signals. The usefulness of the empirical beam model in interpretation and parameterization of film data was demonstrated.

Introduction

The last decade has seen considerable advances in pre-clinical radiotherapy research. Several devices for small animal radiation research have been developed, allowing the delivery of conformal doses in a precise and reproducible fashion [1]. Until recently, small animal radiotherapy research relied on relatively crude methods such as broad-field and whole-body irradiations of test subjects. However, with new small animal radiation therapy platforms, it has become possible to better mimic modern treatment modalities commonly found in the human clinic, such as image guidance, 3D-conformal, and arc deliveries. This is an important step forward in bringing pre-clinical research closer to clinical application.

Modern pre-clinical systems often employ X-rays in the kV energy range for therapy [1]. While this is necessary to minimize penumbrae and build-up effects, which can extend several millimetres for photons in the MV range, it comes with a practical advantage, as X-ray tubes are much cheaper and treatment rooms require less shielding. However, precise dose calculation becomes much harder, as determining water-equivalent thickness for the different tissue types at this energy range is more complex than for MV beams due to a stronger dependence of absorption on tissue composition. Hence, established pre-clinical dose calculation systems capable of providing accurate tissue-dependent dose calculations for small animal radiotherapy treatment using kV beams have yet to be established [1].

Accurate dose calculations for small animal treatment planning and experimental verification measured doses can be performed using Monte Carlo simulations. Unlike most conventional dose calculation engines, Monte Carlo directly includes cross sections for tissue heterogeneities, thereby considerably improving the accuracy of the final dose distribution [2]. Monte Carlo approaches have been chosen by research groups, at John Hopkins [1], [3], Maastricht [4], Toronto [5], and Stanford [6], [7]. The last group managed to achieve a statistical uncertainty of 1%, but a computation time of up to 100 h was needed [6]. Much larger uncertainties would be acceptable for animal radiotherapy treatment. Nevertheless, considerable computation times render Monte Carlo an inconvenient tool for dose calculation, especially in a small-animal laboratory setting. Currently, Monte Carlo in this setting has only involved fairly simple treatment planning, as of now falling short of its potential as a powerful dose calculation tool [1]. Therefore, for practical applications, many groups rely on analytical methods based on the standard beam model to calculate point dose and dose distributions [3], [8], but none of these approaches consider tissue or phantom inhomogeneities. Recently, preliminary results for a convolution-superposition dose calculation system have been reported [9], [10], but they do not contain sufficient experimental verification in heterogeneous media, which is not an easy task.

Verifying a new treatment planning dose calculation model experimentally is especially challenging for small animal radiotherapy, since field beam diameters usually range from 0.5 to 15 mm, making it impossible to rely on more common dosimeters such as ion chambers. Therefore, EBT and EBT2 Gafchromic films have become generally accepted as a means to measure 2D dose distributions under these conditions [3], [11], as they provide the high resolution required for this task. Their high acceptance was increased as they have previously been shown in some studies to be energy-independent for energies ranging from 75 kVp–6 MV [12], which includes the energy ranges used for small animal radiotherapy, though more recent data suggest otherwise [13], [14], [15]. However, Gafchromic film dosimetry for narrow beams (1 mm–100 mm size) is typically associated with relatively large pixel-to-pixel noise, film-to-film variability and poor dynamic range (in measurement of in- vs. out-of-field, shallow vs. deep depths). For this reason, film data analysis requires a beam model-based approach to guide interpretation of the data, especially for heterogeneous media. Until now, empirical beam data in heterogeneous media for extremely narrow kV beams is scarce [3] and there are no empirical models that would help with its characterization.

In view of the above, the aims of this study are: (1) to modify the existing film dosimetry protocol and make it more accurate and efficient in simultaneous processing of many films, and (2) parameterize the obtained data using an empirical beam model for simultaneous homogeneous and inhomogeneous media. For the first goal, we modified the current EBT2 film dosimetry approach for the SARRP [3] to include the new dosimetry approach introduced in Micke et al. [16], which was further studied by other groups [13], [17], with additional modifications of our own, and to increase the number of processed films while removing uncertainties due to scanner non-uniformity and film inhomogeneities. This protocol was then used to generate an extensive film dose database employed for the derivation of beam model parameters. Relative and absolute dose measurements were taken in inhomogeneous media of various settings and were compared against an empirical beam model for a 5 × 5 mm2 field. The model was then determined by experimentally determining the attenuation and scatter of different materials and determining the radiological pathlength through water-equivalent thicknesses.

Section snippets

Phantom material and setup

An overview of the phantoms used in this study can be seen in Fig. 1. Solid water slabs measured 60 × 60 × 5 mm3 and were water-equivalent for kV beams according to the manufacturer (CIRS, Norfolk, VA). Bone-equivalent material (Gammex Inc., Middleton, WI) was cut to measure 50 × 10 × 2 mm3; inflated lung-equivalent material (Gammex Inc., Middleton, WI) had the dimensions 50 × 20 × 10 mm3. The material densities were 1.85 g/cm3 for bone-equivalent material and 0.26 g/cm3 for the inflated

Film dosimetry

Analysis of unexposed films for three different boxes clearly showed that the background signal can vary significantly between separate deliveries even if the films are of the same LOT number and the temperature indicator shows no heat exposure. The results are shown in Table 1.

Figure 3 shows the impact of the correction steps on the calibration curve. Applying the fit to uncorrected data shows that while the curve matches the measured points in the high dose regions with acceptable accuracy,

Film dosimetry

As Fig. 3 indicates, scanner correction and background correction contributed considerably towards improving the accuracy of the results, leading to better fits in the low dose regions for all three channels. While several publications have shown that it is sufficient for EBT2 dosimetry to rely on multi-channel non-uniformity correction alone [13], [16], we found that using the background correction was necessary to remove background signal variations that occurred between different boxes of

Conclusions

We could demonstrate that despite its intrinsic limitations, film dosimetry is a sound approach for 2D dose measurement in the low energy range for small field sizes where a high resolution is required. The modifications introduced to the film dosimetry protocol allow us to evaluate up to nine films in one scan while keeping a high level of accuracy, making it easier to process large numbers of film for experiments and commissioning, about 800 films in the case of this study.

We have shown that

Acknowledgements

Parts of this work have been supported by a grant from the NCI (RO1 CA108449) and a scholarship from the Baden-Württemberg Stiftung, Germany.

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