Cheng Chee W, Das Indra J, Huq M Saiful
Arizona Oncology Associates, Tucson, Arizona 85712, USA.
Med Phys. 2003 Nov;30(11):2959-68. doi: 10.1118/1.1619230.
In the step-and-shoot technique delivery of intensity modulated radiation therapy (IMRT), each static field consists of a number of beamlets, some of which may be very small. In this study, we measured the dose characteristics for a range of field sizes: 2 x 2 to 12 x 10 cm2 for 6 and 15 MV x rays. For a given field length, a number of treatment fields are set up by sequentially increasing the field width using a multi leaf collimator. A set of fields is delivered with the accelerator operated in the IMRT mode. Using an ion chamber, the output factors at 1 cm and 3 cm laterally from a field edge are measured at different depths in a solid water phantom. Our results show that with insufficient lateral distance in at least one direction, the absorbed dose never reaches the equilibrium values, and can be significantly lower for very small field sizes. For example, the output factor of the 2 x 2 cm2 field relative to 10 x 10 cm2 at d(max0 is 0.832 and 0.790 for 6 MV and 15 MV x rays, respectively. Multiple output factor curves are obtained for different field lengths and different buildup conditions. Thus under nonequilibrium conditions, output factors are critically dependent on the field size and the conventional method of determining the equivalent square does not apply. Comparison of output factors acquired in the commissioning of the accelerator with those measured in the present study under conditions of nonequilibrium shows large discrepancies between the two sets of measurements. Thus monitor units generated by a treatment planning system using beam data commissioned with symmetric fields may be underestimated by > 5%, depending on the size and shape of the segments. To facilitate manual MU calculation as an independent check in step-and-shoot IMRT, the concept of effective equivalent square (EES) is introduced. Using EES, output factors can be calculated using existing beam data for fields with asymmetric collimator settings and under conditions of lateral disequilibrium.
在调强放射治疗(IMRT)的静态调强技术中,每个静态野由多个子野组成,其中一些子野可能非常小。在本研究中,我们测量了一系列野大小(6和15 MV X射线的2×2至12×10 cm²)的剂量特性。对于给定的野长度,使用多叶准直器通过依次增加野宽度来设置多个治疗野。一组野在加速器以IMRT模式运行时进行照射。使用电离室,在固体水模体的不同深度测量距野边缘横向1 cm和3 cm处的输出因子。我们的结果表明,在至少一个方向上横向距离不足时,吸收剂量永远不会达到平衡值,对于非常小的野大小,吸收剂量可能会显著降低。例如,2×2 cm²野相对于10×10 cm²野在d(max)处的输出因子,6 MV和15 MV X射线分别为0.832和0.790。针对不同的野长度和不同的建成条件获得了多条输出因子曲线。因此,在非平衡条件下,输出因子严重依赖于野大小,传统的确定等效方的方法不适用。在加速器调试过程中获得的输出因子与本研究在非平衡条件下测量的输出因子进行比较,结果显示两组测量之间存在很大差异。因此,治疗计划系统使用对称野调试的射束数据生成的监测单位可能会被低估>5%,这取决于子野的大小和形状。为便于在静态调强IMRT中作为独立检查进行手动MU计算,引入了有效等效方(EES)的概念。使用EES,可以利用现有射束数据计算非对称准直器设置野和横向非平衡条件下的输出因子。