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1.
Med Phys ; 48(12): 8052-8061, 2021 Dec.
Article in English | MEDLINE | ID: mdl-34668589

ABSTRACT

PURPOSE: To predict and mitigate for the degradation in physical and biologically effective dose distributions of particle beams caused by microscopic heterogeneities in lung tissue. MATERIALS AND METHODS: The TRiP98 treatment planning system was adapted to account for the beam-modulating effect of heterogeneous lung tissue in physical and biological inverse treatment planning. The implementation employs an analytical model that derives the degradation from the established "modulation power" parameter P mod and the total water-equivalent thickness of lung parenchyma traversed by the beam. Beam modulation was reproduced through an on-the-fly convolution of the reference Bragg curve with Gaussian kernels depending on the modulation power of lung tissue (upstream). For biological doses, the degradation was determined by modulating dose-averaged α , ß , and LET distributions. Carbon SOBP measurements behind lung substitute material were performed to validate the code. The implementation was then applied to a phantom and patient case. RESULTS: Experimental results show the passage through a 20-cm Gammex LN300 slab led to a decrease in target coverage and broadening of the SOBP distal fall-off. However, dose coverage was regained through optimization. A good agreement between calculated and measured SOBPs was also found. In addition, a patient case study revealed a 3.2% decrease in D 95 from degradation ( P mod = 450 µ m), which was reduced to a 0.4% difference after optimization. Furthermore, widening of the RBE distribution beyond the target distal edge was observed. This implies an increased degradation in the biological dose, which could be harmful to healthy tissues distal to the target. CONCLUSIONS: This is the first implementation capable of compensating for lung dose perturbations, which is more effective than margin extensions. A larger patient study is needed to examine the observed modulation in the RBE distribution and judge the clinical relevance also in IMPT, where margins might prove insufficient to recover target coverage.


Subject(s)
Heavy Ion Radiotherapy , Proton Therapy , Algorithms , Humans , Lung/diagnostic imaging , Phantoms, Imaging , Radiotherapy Planning, Computer-Assisted , Relative Biological Effectiveness
2.
Int J Radiat Oncol Biol Phys ; 102(5): 1551-1559, 2018 12 01.
Article in English | MEDLINE | ID: mdl-30076985

ABSTRACT

PURPOSE: To investigate the suitability of the linear-quadratic (LQ) and universal survival curve (USC) models in describing the 3-year tumor control probability data of patients with stage I non-small cell lung cancer treated with carbon-ion radiation therapy. Carbon-ion radiation therapy was given at a total dose of 59.4 to 95.4 Gy (relative biological effectiveness [RBE]) in 18 fractions, at 72 Gy[RBE] in 9 fractions, at 52.8 to 60 Gy[RBE] in 4 fractions, and at 28 to 50 Gy[RBE] in a single fraction. METHODS AND MATERIALS: A meta-analysis of published clinical data from 394 patients presenting with early-stage non-small cell lung cancer was conducted. Tumor control probability modeling based on the LQ and USC models was performed by simultaneously fitting the clinical data obtained from the different fractionation schedules while considering several spread-out Bragg peak (SOBP) sizes. Radiobiological parameters were derived from the fit. On the basis of the results, a novel SOBP was created for the single-fraction regimen that was optimized with respect to the USC model and aimed at achieving a 95% local control. RESULTS: The USC model gave a better fit to the 3-year local control data than the LQ model did. The fit using various SOBP sizes yielded transition doses between 5.6 and 7.0 Gy. The results also revealed α/ß ratios between 7.4 and 9.1 Gy for the LQ model and between 7.4 and 9.4 Gy for the USC model. CONCLUSIONS: The USC model provided a better estimate of the local control rate for the single-fraction course. For the schemes with a greater number of fractions, the local control rate estimates from the LQ and USC models were comparable. A USC-based SOBP design was then created for the single-fraction schedule. The updated design resulted in a flatter RBE profile compared with the conventional SOBP design. It also gave a better clinical dose prediction to optimize the tumor control rate.


Subject(s)
Carcinoma, Non-Small-Cell Lung/pathology , Carcinoma, Non-Small-Cell Lung/radiotherapy , Dose Fractionation, Radiation , Heavy Ion Radiotherapy , Lung Neoplasms/pathology , Lung Neoplasms/radiotherapy , Humans , Monte Carlo Method , Neoplasm Staging , Probability , Treatment Outcome
3.
Front Oncol ; 6: 23, 2016.
Article in English | MEDLINE | ID: mdl-26904502

ABSTRACT

The use of charged particle therapy in cancer treatment is growing rapidly, in large part because the exquisite dose localization of charged particles allows for higher radiation doses to be given to tumor tissue while normal tissues are exposed to lower doses and decreased volumes of normal tissues are irradiated. In addition, charged particles heavier than protons have substantial potential clinical advantages because of their additional biological effects, including greater cell killing effectiveness, decreased radiation resistance of hypoxic cells in tumors, and reduced cell cycle dependence of radiation response. These biological advantages depend on many factors, such as endpoint, cell or tissue type, dose, dose rate or fractionation, charged particle type and energy, and oxygen concentration. This review summarizes the unique biological advantages of charged particle therapy and highlights recent research and areas of particular research needs, such as quantification of relative biological effectiveness (RBE) for various tumor types and radiation qualities, role of genetic background of tumor cells in determining response to charged particles, sensitivity of cancer stem-like cells to charged particles, role of charged particles in tumors with hypoxic fractions, and importance of fractionation, including use of hypofractionation, with charged particles.

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