Konijnenberg M W, Dewit L G, Mijnheer B J, Raaijmakers C P, Watkins P R
The Netherlands Cancer Institute, Antoni van Leeuwenhoek Huis, Amsterdam.
Radiat Res. 1995 Jun;142(3):327-39.
Simulation models based on the neutron and photon Monte Carlo code MCNP were used to study the therapeutic possibilities of the HB11 epithermal neutron beam at the High Flux Reactor in Petten. Irradiations were simulated in two types of phantoms filled with water or tissue-equivalent material for benchmark treatment planning calculations. In a cuboid phantom the influence of different field sizes on the thermal-neutron-induced dose distribution was investigated. Various shapes of collimators were studied to test their efficacy in optimizing the thermal-neutron distribution over a planning target volume and healthy tissues. Using circular collimators of 8, 12 and 15 cm diameter it was shown that with the 15-cm field a relatively larger volume within 85% of the maximum neutron-induced dose was obtained than with the 8- or 12-cm-diameter field. However, even for this large field the maximum diameter of this volume was 7.5 cm. In an ellipsoid head phantom the neutron-induced dose was calculated assuming the skull to contain 10 ppm 10B, the brain 5 ppm 10B and the tumor 30 ppm 10B. It was found that with a single 15-cm-diameter circular beam a very inhomogenous dose distribution in a typical target volume was obtained. Applying two equally weighted opposing 15-cm-diameter fields, however, a dose homogeneity within +/- 10% in this planning target volume was obtained. The dose in the surrounding healthy brain tissue is 30% at maximum of the dose in the center of the target volume. Contrary to the situation for the 8-cm field, combining four fields of 15 cm diameter gave no large improvement of the dose homogeneity over the target volume or a lower maximum dose in the healthy brain. Dose-volume histograms were evaluated for the planning target volume as well as for the healthy brain to compare different irradiation techniques, yielding a graphical confirmation of the above conclusions. Therapy with BNCT on brain tumors must be performed either with an 8-cm four-field irradiation or with two opposing 15- or 12-cm fields to obtain an optimal dose distribution.
基于中子和光子蒙特卡罗代码MCNP的模拟模型被用于研究位于佩滕高通量反应堆的HB11超热中子束的治疗可能性。在充满水或组织等效材料的两种类型的体模中进行辐照模拟,以进行基准治疗计划计算。在一个长方体体模中,研究了不同射野大小对热中子诱发剂量分布的影响。研究了各种形状的准直器,以测试它们在优化计划靶体积和健康组织内热中子分布方面的效果。使用直径为8、12和15厘米的圆形准直器表明,与8厘米或12厘米直径的射野相比,15厘米射野在最大中子诱发剂量的85%范围内可获得相对更大的体积。然而,即使对于这个大射野,该体积的最大直径也为7.5厘米。在一个椭球体头部体模中,假设颅骨含10 ppm的硼-10、脑含5 ppm的硼-10以及肿瘤含30 ppm的硼-10,计算中子诱发剂量。发现使用单个直径15厘米的圆形射束时,在典型靶体积中获得的剂量分布非常不均匀。然而,应用两个等权重的相对的直径15厘米的射野时,在这个计划靶体积中获得了±10%以内的剂量均匀性。周围健康脑组织中的剂量最大为靶体积中心剂量的30%。与8厘米射野的情况相反,组合四个直径15厘米的射野并没有在靶体积上显著改善剂量均匀性,也没有降低健康脑组织中的最大剂量。对计划靶体积以及健康脑的剂量体积直方图进行评估,以比较不同的照射技术,从图形上证实了上述结论。脑肿瘤的硼中子俘获治疗必须采用8厘米四野照射或两个相对的15厘米或12厘米射野进行,以获得最佳剂量分布。