Chow James C L, Owrangi Amir M
Department of Radiation Oncology, University of Toronto, Toronto, ON M5G 2M9, Canada; Radiation Medicine Program, Princess Margaret Caner Center, University Health Network, Toronto, ON M5G 2M9, Canada.
Department of Radiation Oncology, University of Toronto, Toronto, ON M5G 2M9, Canada; Department of Medical Physics, Sunnybrook Health Sciences Center, Toronto ON M4N 3M5, Canada.
Rep Pract Oncol Radiother. 2016 Jan-Feb;21(1):63-70. doi: 10.1016/j.rpor.2015.11.001. Epub 2015 Nov 30.
Using flattened and unflattened photon beams, this study investigated the spectral variations of surface photon energy and energy fluence in the bone heterogeneity and beam obliquity.
Surface dose enhancement is a dosimetric concern when using unflattened photon beam in radiotherapy. It is because the unflattened photon beam contains more low-energy photons which are removed by the flattening filter of the flattened photon beam.
We used a water and bone heterogeneity phantom to study the distributions of energy, energy fluence and mean energy of the 6 MV flattened and unflattened photon beams (field size = 10 cm × 10 cm) produced by a Varian TrueBEAM linear accelerator. These elements were calculated at the phantom surfaces using Monte Carlo simulations. The photon energy and energy fluence calculations were repeated with the beam angle turned from 0° to 15°, 30° and 45° in the water and bone phantom.
Spectral results at the phantom surfaces showed that the unflattened photon beams contained more photons concentrated mainly in the low-energy range (0-2 MeV) than the flattened beams associated with a flattening filter. With a bone layer of 1 cm under the phantom surface and within the build-up region of the 6 MV photon beam, it is found that both the flattened and unflattened beams had slightly less photons in the energy range <0.4 MeV compared to the water phantom. This shows that the presence of the bone decreased the low-energy photon backscatters to the phantom surface. When both the flattened and unflattened photon beams were rotated from 0° to 45°, the number of photon and mean photon energy increased. This indicates that both photon beams became more hardened or penetrate when the beam angle increased. In the presence of bone, the mean energies of both photon beams increased. This is due to the absorption of low-energy photons by the bone, resulting in more beam hardening.
This study explores the spectral relationships of surface photon energy and energy fluence with bone heterogeneity and beam obliquity for the flattened and unflattened photon beams. The photon spectral information is important in studies on the patient's surface dose enhancement using unflattened photon beams in radiotherapy.
本研究使用扁平和平坦化光子束,研究了在骨组织不均匀性和射束倾斜情况下表面光子能量和能量注量的光谱变化。
在放射治疗中使用未平坦化光子束时,表面剂量增加是一个剂量学问题。这是因为未平坦化光子束包含更多低能光子,而这些光子会被平坦化光子束的平坦化滤波器去除。
我们使用水和骨组织不均匀性模体,研究了Varian TrueBEAM直线加速器产生的6兆伏扁平和平坦化光子束(射野尺寸 = 10厘米×10厘米)的能量、能量注量和平均能量分布。这些参数是使用蒙特卡罗模拟在模体表面计算得出的。在水模体和骨模体中,将射束角度从0°旋转到15°、30°和45°,重复进行光子能量和能量注量计算。
模体表面的光谱结果表明,与带有平坦化滤波器的平坦化光束相比,未平坦化光子束包含更多主要集中在低能范围(0 - 2兆电子伏)的光子。在模体表面下方1厘米处且在6兆伏光子束的建成区内有一层骨组织时,发现与水模体相比,平坦化和平坦化光子束在能量范围<0.4兆电子伏内的光子都略少。这表明骨组织的存在减少了低能光子向模体表面的反向散射。当平坦化和平坦化光子束都从0°旋转到45°时,光子数量和平均光子能量增加。这表明当射束角度增加时,两种光子束都变得更硬或穿透性更强。在有骨组织的情况下,两种光子束的平均能量都增加。这是由于骨组织吸收了低能光子,导致更多的射束硬化。
本研究探讨了扁平和平坦化光子束在骨组织不均匀性和射束倾斜情况下表面光子能量和能量注量的光谱关系。光子光谱信息在放射治疗中使用未平坦化光子束研究患者表面剂量增加方面很重要。