Oldham M, Baustert I, Lord C, Smith T A, McJury M, Warrington A P, Leach M O, Webb S
Joint Department of Physics, Institute of Cancer Research and the Royal Marsden NHS Trust, Sutton, Surrey, UK.
Phys Med Biol. 1998 May;43(5):1113-32. doi: 10.1088/0031-9155/43/5/005.
BANG-gel dosimetry offers the potential for measuring the dose delivered by a radiotherapy treatment technique, in three dimensions, with high spatial resolution and good accuracy. The ability to measure comprehensively a 3D dose distribution is a major advantage of the gel dosimeter over conventional planar and point-based dosimeter devices, particularly when applied to the verification of complex dose distributions characteristic of intensity-modulated radiotherapy (IMRT). In this paper an in-house manufactured BANG-gel dosimeter was applied to study the dose distributions of two irradiation experiments for which the distributions were known: (i) a dosimetrically simple parallel-opposed irradiation, and (ii) a more complex nine-field 'static tomotherapy' intensity-modulated irradiation delivered with the Nomos MIMiC. The uniform distribution in (i) allowed a study of the magnetic resonance (MR) imaging parameters to achieve an optimal trade-off between noise and image resolution (optimum image resolution for the Siemens 1.5T Vision system was determined to be approximately 0.8 mm2 with a slice thickness of 2 mm). The spatial uniformity of gel sensitivity to radiation was found to depend strongly on the presence of oxygen, which must be eliminated for the gel dosimeter to be of use. The gel dosimeter was found to agree well with predicted dose distributions and accurately measured the steep penumbral fall-off of dose, even after many days, proving its potential for the verification of IMRT distributions. In the nine-field IMRT delivery (ii) the predicted dose was computed by both an in-house 'component-delivery' dose algorithm and the Peacock planning-system dose algorithm. Good agreement was found between the two algorithms despite the latter's omission of the change in penumbral characteristics with aperture-size during delivery, lack of inhomogeneity correction and approximate modelling of leaf leakage. These effects were found to be small for the problem studied. The predicted distribution agreed well with the gel-measured distribution at medium and high doses (50-90% isodose lines) although differences of up to 10% were observed at lower doses (30% isodose line). The gel dosimeter was found to have the potential to verify IMRT distributions but required considerable care to achieve accurate results. Attention was required to achieve uniformity of gel sensitivity (to prevent oxygen contamination), and in the calibration process.
BANG凝胶剂量测定法能够在三维空间中以高空间分辨率和良好的准确性测量放射治疗技术所传递的剂量。与传统的平面和基于点的剂量计设备相比,凝胶剂量计能够全面测量三维剂量分布,这是其主要优势,特别是在应用于验证调强放射治疗(IMRT)特有的复杂剂量分布时。在本文中,一种自制的BANG凝胶剂量计被用于研究两个已知剂量分布的照射实验:(i)剂量学上简单的对穿照射,以及(ii)使用Nomos MIMiC进行的更复杂的九野“静态断层放射治疗”调强照射。(i)中的均匀分布使得能够研究磁共振(MR)成像参数,以在噪声和图像分辨率之间实现最佳权衡(确定西门子1.5T Vision系统的最佳图像分辨率约为0.8平方毫米,切片厚度为2毫米)。发现凝胶对辐射的敏感性的空间均匀性强烈依赖于氧气的存在,为了使凝胶剂量计能够使用,必须消除氧气。发现凝胶剂量计与预测的剂量分布吻合良好,即使在许多天后也能准确测量剂量的陡峭半影下降,证明了其在验证IMRT分布方面的潜力。在九野IMRT照射(ii)中,预测剂量由内部的“成分传递”剂量算法和孔雀计划系统剂量算法计算得出。尽管后者在照射过程中忽略了半影特征随孔径大小的变化、缺乏不均匀性校正以及对叶片泄漏的近似建模,但两种算法之间仍发现了良好的一致性。对于所研究的问题,发现这些影响较小。预测分布在中高剂量(50 - 90%等剂量线)下与凝胶测量分布吻合良好,尽管在较低剂量(30%等剂量线)下观察到高达10%的差异。发现凝胶剂量计有潜力验证IMRT分布,但需要相当小心才能获得准确结果。在实现凝胶敏感性均匀性(防止氧气污染)以及校准过程中都需要注意。