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Published on: March 11, 2021
Alpha dose modeling in diffusing alpha-emitters radiation therapy-Part I: single-seed calculations in one and two
Guy Heger1, Arindam Roy1, Mirta Dumančić1
1Unit of Nuclear Engineering, Faculty of Engineering Sciences, Ben-Gurion University of the Negev, Be'er-Sheva, Israel.
This study refines the Diffusion-Leakage (DL) model for Diffusing alpha-emitters Radiation Therapy (DaRT) dose calculations. A 2D model is recommended for treatment planning, while a 1D model offers efficiency for lattice studies.
Area of Science:
- Medical Physics
- Radiation Oncology
- Nuclear Medicine
Background:
- Diffusing alpha-emitters Radiation Therapy (DaRT) utilizes alpha particles for solid tumor treatment.
- DaRT involves interstitial seeds releasing alpha emitters that diffuse within the tumor.
- Accurate alpha dose calculations require advanced modeling of atom transport.
Purpose of the Study:
- To extend the Diffusion-Leakage (DL) model to realistic DaRT seed geometries.
- To develop and validate computational models for DaRT dose calculations.
- To provide guidance for treatment planning in clinical DaRT trials.
Main Methods:
- Derived a closed-form asymptotic solution for a cylindrical alpha source.
- Developed a 1D finite-element numerical scheme for time-dependent dose calculations.
- Investigated a 2D axisymmetric scheme for finite seed geometries.
Main Results:
- Approximating seeds as line sources underestimates alpha dose compared to 2D calculations.
- The 1D time-dependent solution closely matches the 2D solution in the seed midplane.
- The 1D solution maintains accuracy within a few percent up to 2 mm from the seed edge.
Conclusions:
- A full 2D solution is necessary for generating accurate dose lookup tables for DaRT treatment planning.
- The 1D solution is suitable for efficient parametric studies of DaRT seed lattices.
- This work provides essential tools for advancing DaRT clinical applications.
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Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
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