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首页> 外文期刊>Journal of radiation research >Correlation between target volume and electron transport effects affecting heterogeneity corrections in stereotactic body radiotherapy for lung cancer
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Correlation between target volume and electron transport effects affecting heterogeneity corrections in stereotactic body radiotherapy for lung cancer

机译:肺癌立体定向放疗中靶标量与影响异质性校正的电子传输效应之间的相关性

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Under Institutional Review Board (IRB) exemption, we retrospectively analyzed the treatment plans of 74 patients with lung cancer who were treated with SBRT at Indiana University School of Medicine, Indianapolis. There were 22 and 52 cases in the right- and left-lobe of the lung, respectively. Details of the prescribed doses for these patients are listed in Table 1. Every SBRT patient was immobilized using either an Elekta Stereotactic Body Frame (Elekta, Stockholm, Sweden) or a CIVCO Body Pro-Lok system (CIVCO, Kalona, IA), depending upon the patient size, comfort and suitability as decided at the time of simulation. Eclipse version 10.0 was used for the treatment planning. Plans were generated to cover 95% of the PTV with the prescribed dose, thus providing typically a 25% higher dose to the GTV. Eclipse provides two algorithms for heterogeneity correction; pencil beam convolution (PBC) and AAA. The PBC model in Eclipse is mainly for homogenous medium (water) dose calculation that gets supplemented with older models modified Batho, Batho power law and equivalent tissue air ration (ETAR) [18]. It was noted that both modified Batho and Batho power law gave almost the same results for SBRT, and hence default modified Batho with PBC was used. The ETAR option with PBC cannot be used with non-coplanar field arrangements, thus ETAR was not an option in this study as the majority of the SBRT fields were non-coplanar. Heterogeneity correction was applied to all clinically approved plans using an AAA algorithm. The AAA is considered a superior algorithm compared with older and pencil beam algorithms [7, 19–21]. Two additional plans were generated for each patient: (i) a treatment plan with no correction (NC), and (ii) PBC with modified Batho heterogeneity correction. In the PBC algorithm, the dose deposited at a point was calculated as a convolution of energy fluence, or total energy released per unit mass (TERMA), with the respective dose deposition kernel pre-calculated for a narrow beam in water [22]. The Batho power-law correction method is an empirical correction to account for both primary beam attenuation and scatter changes in heterogeneous materials. The modified Batho correction uses only the descending part of the TAR/TMR curve because the curve in the build-up region of a high-energy photon is no longer valid. However, PBC does not take into account changes in lateral electron transport. This provided us with an opportunity to differentiate between photon attenuation (PBC) versus electron transport (AAA). JMP software (ver. 9.0.2; SAS Institute, Cary, NC) was used for statistical analysis. All pairwise comparisons among the three calculation algorithms were conducted for the isocenter dose (DIso), D95% and V100% using the Steel–Dwass test. The correlation between dosimetric parameters and anatomical characteristics including ΔPL, the PTV and the distance between the PTV and the chest wall or mediastinum was assessed with Spearman's rank correlation coefficient. Statistical significance was defined as a P-value 0.05. The DIso relative to the prescribed dose for each plan is shown in Fig. 3a. The DIso (average ± SD) for the entire patient population was 110.8 ± 4.4%, 132.6 ± 4.3% and 124.2 ± 3.1% for NC, PBC and AAA, respectively. The ΔDIso calculated with PBC and AAA were larger than that calculated with NC by 21.8% and 13.4%, respectively, in our population, with both P 0.0001. The DIso of AAA was 8.4% smaller than that of PBC (P 0.0001). In Fig. 3b, the isocenter dose difference (ΔDIso) between the dose with and without heterogeneity corrections of PBC (ΔPBC) and AAA (ΔAAA) were plotted with ΔPL as shown in Eq 1. The slope of the lines for PBC and AAA are nearly identical. The ΔPBC and ΔAAA showed intermediate linear correlation with ΔPL (ρ = 0.60, P 0.0001 for both). Typically, patients are treated with better than 95% target coverage, as shown in Fig. 4a indicating V100% with NC, PBC and AAA algorithms for all patients. The median V100% was 90.6% (range, 42.3–98.7%), 100.0% (range, 92.9–100.0%) and 96.0% (range, 75.6–99.9%) for NC, PBC and AAA, respectively. The long error bars indicate the variability among the patients. The average ± SD of D95% was 97.6 ± 5.0%, 114.6 ± 7.4% and 100.5 ± 2.8% for NC, PBC and AAA, respectively as shown in Fig. 4b. The D95% of PBC and AAA were larger than that of NC by 17.0% (P 0.0001) and 2.9% (P 0.0001), respectively. The ΔD95% of AAA plans was 14.1% smaller than that of PBC (P 0.0001). Figure 4c illustrates the evaluation of ΔD95% of the PTV for each patient, representing a similar analysis to that of Fig.3b for DIso. The ΔPBC shows intermediate linear correlation with ΔPL (ρ = 0.58, P 0.0001), although ΔAAA showed weaker correlation with ΔPL (ρ = 0.41, P = 0.0003
机译:在机构审查委员会(IRB)豁免下,我们回顾性分析了印第安纳波利斯印第安纳大学医学院接受SBRT治疗的74例肺癌患者的治疗计划。肺右叶和左叶分别有22例和52例。这些患者的处方剂量详细信息列于表1。根据具体情况,每位SBRT患者均使用Elekta立体定向车架(Elekta,斯德哥尔摩,瑞典)或CIVCO Body Pro-Lok系统(CIVCO,Kalona,IA)进行固定。在模拟时决定患者的大小,舒适度和适用性。 Eclipse 10.0版用于治疗计划。制定计划以规定的剂量覆盖95%的PTV,因此通常为GTV提供25%的剂量。 Eclipse提供了两种用于异质性校正的算法;铅笔束卷积(PBC)和AAA。 Eclipse中的PBC模型主要用于均质介质(水)剂量计算,并补充有改进的Batho,Basto幂定律和等效组织空气定量(ETAR)的较旧模型[18]。值得注意的是,修改后的Batho和Batho幂定律对于SBRT都给出了几乎相同的结果,因此使用了默认的修改后的Batho和PBC。具有PBC的ETAR选项不能与非共面的场布置一起使用,因此,由于大多数SBRT场都是非共面的,因此在本研究中ETAR不是选项。使用AAA算法将异质性校正应用于所有临床批准的计划。与旧的和笔形波束算法相比,AAA被认为是一种更好的算法[7,19-21]。为每个患者生成了两个其他计划:(i)不进行校正的治疗计划(NC),以及(ii)具有改良的Batho异质性校正的PBC。在PBC算法中,在某一点沉积的剂量被计算为能量通量或每单位质量释放的总能量(TERMA)的卷积,并预先计算了水中的窄束[22]。 Batho幂律校正方法是一种经验校正,可同时考虑主光束衰减和异质材料中的散射变化。修改后的Batho校正仅使用TAR / TMR曲线的下降部分,因为高能光子堆积区域中的曲线不再有效。但是,PBC没有考虑横向电子传输的变化。这为我们提供了区分光子衰减(PBC)与电子传输(AAA)的机会。使用JMP软件(9.0.2版; SAS Institute,Cary,NC)进行统计分析。使用Steel对三种计算算法的等中心点剂量(D Iso ),D 95%和V 100%进行了所有成对比较。 –Dwass测试。用Spearman秩相关系数评估剂量参数与解剖特征(包括ΔPL,PTV和PTV与胸壁或纵隔之间的距离)之间的相关性。统计显着性定义为P值<0.05。每个计划相对于规定剂量的D Iso 表示在图3a中。 NC,PBC和AAA的整个患者群体的D Iso (平均值±SD)分别为110.8±4.4%,132.6±4.3%和124.2±3.1%。用PBC和AAA计算的ΔD Iso 在我们的人群中分别比用NC计算的ΔD Iso 大21.8%和13.4%,两者均P <0.0001。 AAA的D 比PBC小8.4%(P <0.0001)。在图3b中,如等式1所示,用ΔPL绘制了有无PBC(ΔPBC)和AAA(ΔAAA)的异质性校正的剂量之间的等中心剂量差(ΔD Iso )。 PBC和AAA的生产线几乎相同。 ΔPBC和ΔAAA与ΔPL表现出中间线性相关性(两者均ρ= 0.60,P <0.0001)。通常,对患者的目标覆盖率要好于95%,如图4a所示,对于所有患者,NC,PBC和AAA算法表明V 100%。 NC,PBC和VBC的中位数V 100%分别为90.6%(范围42.3–98.7%),100.0%(范围92.9–100.0%)和96.0%(范围75.6–99.9%)。 AAA。较长的误差线指示患者之间的变异性。如图4b所示,NC,PBC和AAA的D 95%的平均±SD分别为97.6±5.0%,114.6±7.4%和100.5±2.8%。 PBC和AAA的D 95%分别比NC大17.0%(P <0.0001)和2.9%(P <0.0001)。 AAA计划的ΔD 95%比PBC小14.1%(P <0.0001)。图4c说明了对每个患者的PTV的ΔD 95%的评估,与图3b对D Iso 的分析相似。 ΔPBC与ΔPL呈中间线性相关(ρ= 0.58,P <0.0001),尽管ΔAAA与ΔPL呈弱相关(ρ= 0.41,P = 0.0003)

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