| Literature DB >> 30845263 |
Yuliang Huang1, Sha Li2, Haizhen Yue1, Meijiao Wang1, Qiaoqiao Hu1, Haiyang Wang1, Tian Li1, Chenguang Li1, Hao Wu1, Yibao Zhang1.
Abstract
The interactive adjustment of the optimization objectives during the treatment planning process has made it difficult to evaluate the impact of beam quality exclusively in radiotherapy. Without consensus in the published results, the arbitrary selection of photon energies increased the probability of suboptimal plans. This work aims to evaluate the dosimetric impact of various photon energies on the sparing of normal tissues by applying a preconfigured knowledge-based planning (RapidPlan) model to various clinically available photon energies for rectal cancer patients, based on model-generated optimization objectives, which provide a comparison basis with less human interference. A RapidPlan model based on 81 historical VMAT plans for pre-surgical rectal cancer patients using 10MV flattened beam (10X) was used to generate patient-specific objectives for the automated optimization of other 20 patients using 6X, 8X, 10X (reference), 6MV flattening-filter-free (6F) and 10F beams respectively on a TrueBeam accelerator. It was observed that flattened beams produced very comparable target dose coverage yet the conformity index using 6F and 10F were clinically unacceptable (>1.29). Therefore, dose to organs-at-risk (OARs) and normal tissues were only evaluated for flattened beams. RapidPlan-generated objectives for 6X and 8X beams can achieve comparable target dose coverage as that of 10X, yet the dose to normal tissues increased monotonically with decreased energies. Differences were statistically significant except femoral heads. From the radiological perspective of view, higher beam energy is still preferable for deep seated tumors, even if multiple field entries such as VMAT technique can accumulate enough dose to the target using lower energies, as reported in the literature. In conclusion, RapidPlan model configured for flattened beams cannot optimize un-flattened beams before adjusting the target objectives, yet works for flattened beams of other energies. For the investigated 10X, 8X and 6X photons, higher energies provide better normal tissue sparing.Entities:
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Year: 2019 PMID: 30845263 PMCID: PMC6405245 DOI: 10.1371/journal.pone.0213271
Source DB: PubMed Journal: PLoS One ISSN: 1932-6203 Impact factor: 3.240
Tumor volumes [cm3] of 81 training cases and 20 validation cases.
| PTVboost | PTV | |||
|---|---|---|---|---|
| Training | Validation | Training | Validation | |
| Mean | 179.54 | 170.70 | 1207.99 | 1151.71 |
| Standard deviation | 92.00 | 96.85 | 165.91 | 187.73 |
| Minimum | 53.31 | 60.5 | 844.12 | 802.40 |
| Maximum | 618.09 | 478.2 | 1675.05 | 1562.00 |
Fig 1The target DVHs of 20 patients, as optimized automatically using various photon energies.
Subfigures (a-d) present the target DVHs of 6X, 6F, 8X and 10 F (dotted lines) relative to the reference 10X results (solid lines) respectively. The figure-in-figure shows the corresponding mean target DVHs of 20 patients, as optimized using the same beam energy.
Dosimetric statistics of OARs comparing the results of 6X and 8X against 10X.
| 6X | 10X | 8X | |||
|---|---|---|---|---|---|
| Urinary bladder | |||||
| V40Gy | 14.19 | 13.37 | 13.98 | ||
| V45Gy | 3.23 | 3.24 | 3.10 | ||
| Dmean | 24.30 | 22.86 | 23.68 | ||
| P | <0.01 | <0.01 | |||
| Femoral heads | |||||
| V40Gy | 0 | 0.01 | 0 | ||
| V45Gy | 0 | 0 | 0 | ||
| Dmean | 13.58 | 13.00 | 13.40 | ||
| P | 0.32 | 0.50 | |||
| NTID | |||||
| Dmean | 17.92 | 17.27 | 17.41 | ||
| P | <0.01 | 0.02 | |||
| Skin | |||||
| Dmean | 10.80 | 9.66 | 9.99 | ||
| P | <0.01 | <0.01 | |||
| Small bowel | |||||
| V35Gy | 7.10 | 5.52 | 6.61 | ||
| V40Gy | 1.09 | 0.67 | 1.01 | ||
| V45Gy | 0 | 0 | 0 | ||
| Dmean | 22.78 | 21.42 | 22.28 | ||
| P | <0.01 | <0.01 | |||
P values were calculated for the mean dose. The units for the volume and dose are % and Gy respectively. Abbreviations: VxGy = volume receiving at least x Gy dose; Dmean = mean dose; NTID = normal tissue integral dose.
Fig 2The DVH differences of the OARs as optimized using various beam energies relative to 10X photons.
The dashed lines plot the data of 20 patients, and the solid lines are their average. The left and right column shows the results of 6X-10X and 8X-10X respectively. Subfigures (a-b), (c-d), (e-f), (g-h) and (i-j) plot the results for the urinary bladder, femoral heads, NTID, skin and small bowel respectively.