Abstract
Purpose
The aim of this study is to investigate an implementation method and the results of a voxel-based self-adaptive prescription dose optimization algorithm for intensity-modulated radiotherapy.
Materials and methods
The self-adaptive prescription dose optimization algorithm used a quadratic objective function, and the optimization engine was implemented using the molecular dynamics. In the iterative optimization process, the optimization prescription dose changed with the relationship between the initial prescription dose and the calculated dose. If the calculated dose satisfied the initial prescription dose, the optimization prescription dose was equal to the calculated dose; otherwise, the optimization prescription dose was equal to the initial prescription dose. We assessed the performance of the self-adaptive prescription dose optimization algorithm with two cases: a mock head and neck case and a breast case. Isodose lines, dose–volume histogram, and dosimetric parameters were compared between the conventional molecular dynamics optimization algorithm and the self-adaptive prescription dose optimization algorithm.
Results
The self-adaptive prescription dose optimization algorithm produces the different optimization results compared with the conventional molecular dynamics optimization algorithm. For the mock head and neck case, the planning target volume (PTV) dose uniformity improves, and the dose to organs at risk is reduced, ranging from 1 to 4%. For the breast case, the use of self-adaptive prescription dose optimization algorithm also leads to improvements in the dose distribution, with the dose to organs at risk almost unchanged.
Conclusion
The self-adaptive prescription dose optimization algorithm can generate an ideal clinical plan more effectively, and it could be integrated into a treatment planning system after more cases are studied.
1 Introduction
Compared with conventional conformal radiotherapy, intensity modulated radiotherapy (IMRT) increases the dose of tumor and decreases the dose of organs by adjusting the intensity distribution of radiation field [1,2,3,4]. IMRT is the mainstream of radiotherapy technology at present. Inverse planning is the foundation of IMRT, and its performance determines the success of IMRT [5,6]. There are two kinds of inverse optimization techniques in IMRT: organ-based optimization and voxel-based optimization. In the organ-based optimization, the prescription dose and weight parameters are given to the organ, and all the voxels in an organ are combined and treated equally in the objective function. Because there is no clear relationship between the dose and weight parameters and the final dose distribution, the determination of these parameters is essentially a “guessing game;” therefore, many trial-and-error are needed, and the plan quality heavily depends on the clinical experience of the planner [7,8]. On the contrary, voxel-based optimization directly adjusts the parameters related to each voxel in the objective function [9,10,11,12]. Previous studies showed that compared with organ-based optimization, voxel-based optimization obtained better dose distribution [13,14,15,16,17,18].
One of the practical difficulties in the voxel-based optimization model is that the number of adjustable parameters increases dramatically, and therefore it is difficult to adjust them manually. In this study, a new algorithm is introduced to automatically adjust the dose prescription of voxels in the optimization process. We call it the voxel-based self-adaptive prescription dose optimization algorithm (SAPDOA). Two cases were used to evaluate the SAPDOA performance.
2 Materials and methods
2.1 Self-adaptive prescription dose optimization algorithm
The optimization engine in this study was molecular dynamics. The implementation detail of conventional molecular dynamics optimization algorithm (CMDOA) has been reported in references, and therefore it is only briefly introduced here [19,20,21]. The CMDOA used a weighted quadratic objective function defined by
where is the objective function, is the beamlet intensity, is the total number of organs, w i is the penalty weight, is the calculated dose, and is the prescribed dose.
The was calculated through the formula given in equation (2):
where is the total number of beamlet, and is the dose contribution matrix of one-unit beamlet intensity.
The SAPDOA also used the weighted quadratic objective function, which was the same as the CMDOA we have implemented, but the objective function was redefined as follows:
where is the total number of voxels, and is the self-adaptive prescription dose.
In CMDOA, the did not change with the number of iterations. However, the may change at every step of the optimization iteration in SAPDOA. The change of follows the following rules:
For the target volume, if the was within a certain range (±5%) of the prescription dose , , else .
For an organ at risk (OAR) volume, if the was smaller than the prescription dose , , else .
Rule 1 allowed us to improve the dose uniformity of the target volume, and rule 2 to avoid the problem of low planning quality caused by excessive prescription dose of OARs.
2.2 Test cases
We evaluated the SAPDOA algorithm with two cases, one of them was from the AAPM TG-119 (mock head and neck) [22], and the other one was a clinical case (breast). We first used the CMDOA to make a reasonable plan (C-plan), and then we used the SAPDOA to get a new plan (S-plan). To make a fair comparison of the two plans, we kept all optimization parameters unchanged except the optimization algorithm. The test process was carried out on the Fonics (Qilin Company, Chengdu, China) treatment planning system (TPS).
For the mock head and neck case, nine 6 MV IMRT beams at 0°, 40°, 80°, 120°, 160°, 200°, 240°, 280°, and 320° were chosen. The dose prescription was PTV D 90% = 50 Gy. The evaluation parameters including D 99% and D 20% for PTV and D 50% for normal structures were used for parotid, and maximum dose was used for cord. In the breast case, a setup with four 6 MV IMRT beams at 122°, 135°, 295°, and 342° was used. The dose prescription was PTV D 97% = 50 Gy. The sensitive structures included lung and heart. We first assessed the plan quality by the dose volume histogram (DVH) for the two cases, and then dosimetric parameters were used to evaluate the difference between the plans using different optimization algorithms. To facilitate the plan comparison, all plans were normalized to the dose prescription.
3 Results and discussion
Figure 1 compares the DVHs for the mock head and neck plan optimized with SAPDOA and CMDOA. The PTV coverage is the same (D 90% = 50 Gy), but the sparing of OARs is greatly improved; especially in the high-dose regions, the dose of OARs of S-plan was obviously decreased. Figure 2(a) and (b) shows the isodose curves for the mock head and neck case optimized with SAPDOA and CMDOA, respectively. It is clearly seen that dose uniformity and conformity of PTV are also improved by adjusting the voxel prescription dose in the iterative optimization process. In addition, the over-dose area is obviously decreased in PTV. In particular, the maximum dose to the spinal cord is reduced. Moreover, there is a ∼10% reduction in the parotid D 50%. The detailed dosimetric parameters are presented in Table 1.

DVHs of the mock head and neck plans obtained using the self-adaptive prescription dose optimization algorithm (solid curves) and the CMDOA (dashed curves).

Isodose curves for the two cases: (a) and (b) are the isodose curves for the mock head and neck case optimized with SAPDOA and CMDOA, respectively; (c) and (d) are the isodose curves for the breast case optimized with SAPDOA and CMDOA, respectively. The isodose lines from the isocenter to the exterior are 110% (orange), 100% (red), 80% (pink), 60% (yellow), and 40% (green) of prescription dose, respectively.
Dosimetric parameters of the mock head and neck case
Parameter | Plan goal (Gy) | Weight | SAPDOA (Gy) | CMDOA (Gy) |
---|---|---|---|---|
HN PTV D 90% | >50 | 10 | 50 | 50 |
HN PTV D 99% | >46.5 | 10 | 46.9 | 45.5 |
HN PTV D 20% | <55 | 10 | 52.6 | 54.8 |
Cord maximum | <40 | 20 | 33.6 | 35.5 |
Left parotid D 50% | <20 | 30 | 19.4 | 21.5 |
Right parotid D 50% | <20 | 20 | 18.5 | 20.6 |
For the breast case, a comparison of DVHs between the C-plan and the S-plan is shown in Figure 3. In this case, the DVH curve of the S-plan is improved. The CMDOA might cause excessive constraints on the target and OARs, which makes it difficult to meet all the optimization objectives. In the SAPDOA proposed in this article, the prescribed dose is automatically adjusted according to the calculated dose in the iteration process of optimization. The SAPDOA balanced the prescribed dose between the target and OARs and avoided the situation of over-constraints on the target and OARs effectively.

DVHs of the breast plans obtained using the self-adaptive prescription dose optimization algorithm (solid curves) and the CMDOA (dashed curves).
Figure 2(c) and (d) shows that the S-plan leads to an increased dose homogeneity and dose conformity within the target, and the over-dose area disappeared compared with the C-plan. The low-dose delivered to the left lung and heart has a tiny difference, ranging from −2.8 to 1.2%. However, the S-plan has a significant improvement for the OARs at the high-dose region (>45 Gy). The detailed dosimetric parameters are presented in Table 2.
Dosimetric parameters of the breast case
Parameter | Plan goal | Weight | SAPDOA | CMDOA |
---|---|---|---|---|
PTV D 97% | >50 Gy | 30 | 50 Gy | 50 Gy |
PTV D 99% | >48.5 Gy | 30 | 48.6 Gy | 48.6 Gy |
PTV D 5% | <54 Gy | 10 | 53.2 Gy | 56.0 Gy |
Left lung V20 | <25% | 30 | 24.4% | 23.5% |
Left lung V5 | <40% | 10 | 33.4% | 35.7% |
Right lung V5 | <1% | 20 | 0.5% | <0.5% |
Heart V30 | <20% | 20 | 18.9% | 18.4% |
Heart V5 | <40% | 10 | 37.8% | 38.1% |
Generally speaking, it is difficult for a treatment plan to meet the dosimetric requirements of target and OARs simultaneously. Therefore, it is usually necessary to adjust the optimization objectives many times to obtain an acceptable compromise solution. At this stage, organ-based inverse optimization is widely used in clinical practice. In organ-based inverse optimization, adding more dose–volume constraints can improve the plan quality, but it cannot change and expand the accessible solution space. Therefore, it is difficult to find a better solution. Different from this is that voxel-based inverse optimization increases the accessible solution space [23]. Many study results showed that compared with the organ-based optimization method, the voxel-based inverse optimization method is easier to obtain qualified plans.
In general, there are two ways to adjust the objective function in voxel-based inverse optimization: one is to change the penalty weight of each voxel, and the other is to adjust the prescription dose of each voxel. Zarepisheh et al. [24] proposed a DVH guided intensity-modulated optimization algorithm that automatically adjusted the weight of voxels, and they applied the new algorithm to a head and neck case and a prostate case. The results showed that the voxel-based model is able to improve the plan quality in terms of the DVH at the reasonable price by exploring the parts of the Pareto surface missing in the organ-based models. Li et al. [8] developed an automatic two-loop algorithm to perform re-optimization of a treatment plan on the patient’s new geometry by considering the original DVH as guidance. Automatic voxel weighting factor adjustments avoided tedious trial-and-error schemes, and it is easier to find an acceptable compromise among different structures for re-planning. Lougovski et al. [25] established an inverse planning framework with the voxel-specific penalty. Substantial improvements were achieved in the final dose distribution by adjusting voxel prescriptions iteratively to boost the region where large mismatch between the actual calculated and desired doses occurs. Wu et al. [26] studied the two different modification schemes (weighting factors/dose prescription) based on Rustem’s quadratic programming algorithms. Case studies demonstrated that the two modification schemes had the capability to fine-tune treatment plans.
In this study, our solution is to first determine the organ weight based on clinical experience, and then automatically determine the prescription dose according to the dose calculated in the iterative process. It can be seen from Section 2 that the principle of the SAPDOA algorithm is simple, and it is easily implementable in any existing inverse planning platform. The SAPDOA was tested on a head and neck case and a breast case. As compared with the CMDOA, the PTV experiences improved dose uniformity and the doses to OARs are also reduced. These results show that the SAPDOA provides room for further improvements of currently achievable dose distributions. Our approach could be integrated into a TPS after more case studies.
We acknowledge that the penalty weight of the SAPDOA is determined and adjusted by the planner based on his clinical experience, which limits the algorithm’s ability to find the optimal solution in a larger solution space. The plan optimized by the algorithm finds the solution space corresponding to the set of penalty weight factors, and therefore the optimized plan may not be the global optimal solution. We are introducing an automatic optimization algorithm that combines voxel prescription dose optimization and penalty weight optimization, so as to effectively expand the solution space, navigate in the expanded solution space, and find the global optimal scheme. We hope that the research results could be published in the following years.
4 Conclusion
Although organ-based inverse optimization is widely used in clinical practice at present, the quality of the plan obtained by organ-based optimization heavily depends on the experience of the planner. The continuous trial-and-error process also leads to the inefficiency of planning. In this study, we investigated a new inverse optimization algorithm, SAPDOA, in IMRT. The results of the two test cases show that this algorithm can more effectively generate an ideal clinical plan. The SAPDOA algorithm is easy to implement on any existing inverse programming platform, and it could be integrated into a 3D TPS after studying more cases.
Acknowledgments
The authors sincerely thank all the teachers who helped in the process of this article.
-
Funding information: This work was supported by the National Key Research and Development Programme of China (grant no. 2016YFC0105103).
-
Conflict of interest: The authors declare that there is no conflict of interest.
References
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© 2021 Chuou Yin et al., published by De Gruyter
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- Position-dependent finite symmetric mass harmonic like oscillator: Classical and quantum mechanical study
- Application of Fibonacci heap to fast marching method
- An analytical investigation of the mixed convective Casson fluid flow past a yawed cylinder with heat transfer analysis
- Considering the effect of optical attenuation on photon-enhanced thermionic emission converter of the practical structure
- Fractal calculation method of friction parameters: Surface morphology and load of galvanized sheet
- Charge identification of fragments with the emulsion spectrometer of the FOOT experiment
- Quantization of fractional harmonic oscillator using creation and annihilation operators
- Scaling law for velocity of domino toppling motion in curved paths
- Frequency synchronization detection method based on adaptive frequency standard tracking
- Application of common reflection surface (CRS) to velocity variation with azimuth (VVAz) inversion of the relatively narrow azimuth 3D seismic land data
- Study on the adaptability of binary flooding in a certain oil field
- CompVision: An open-source five-compartmental software for biokinetic simulations
- An electrically switchable wideband metamaterial absorber based on graphene at P band
- Effect of annealing temperature on the interface state density of n-ZnO nanorod/p-Si heterojunction diodes
- A facile fabrication of superhydrophobic and superoleophilic adsorption material 5A zeolite for oil–water separation with potential use in floating oil
- Shannon entropy for Feinberg–Horodecki equation and thermal properties of improved Wei potential model
- Hopf bifurcation analysis for liquid-filled Gyrostat chaotic system and design of a novel technique to control slosh in spacecrafts
- Optical properties of two-dimensional two-electron quantum dot in parabolic confinement
- Optical solitons via the collective variable method for the classical and perturbed Chen–Lee–Liu equations
- Stratified heat transfer of magneto-tangent hyperbolic bio-nanofluid flow with gyrotactic microorganisms: Keller-Box solution technique
- Analysis of the structure and properties of triangular composite light-screen targets
- Magnetic charged particles of optical spherical antiferromagnetic model with fractional system
- Study on acoustic radiation response characteristics of sound barriers
- The tribological properties of single-layer hybrid PTFE/Nomex fabric/phenolic resin composites underwater
- Research on maintenance spare parts requirement prediction based on LSTM recurrent neural network
- Quantum computing simulation of the hydrogen molecular ground-state energies with limited resources
- A DFT study on the molecular properties of synthetic ester under the electric field
- Construction of abundant novel analytical solutions of the space–time fractional nonlinear generalized equal width model via Riemann–Liouville derivative with application of mathematical methods
- Some common and dynamic properties of logarithmic Pareto distribution with applications
- Soliton structures in optical fiber communications with Kundu–Mukherjee–Naskar model
- Fractional modeling of COVID-19 epidemic model with harmonic mean type incidence rate
- Liquid metal-based metamaterial with high-temperature sensitivity: Design and computational study
- Biosynthesis and characterization of Saudi propolis-mediated silver nanoparticles and their biological properties
- New trigonometric B-spline approximation for numerical investigation of the regularized long-wave equation
- Modal characteristics of harmonic gear transmission flexspline based on orthogonal design method
- Revisiting the Reynolds-averaged Navier–Stokes equations
- Time-periodic pulse electroosmotic flow of Jeffreys fluids through a microannulus
- Exact wave solutions of the nonlinear Rosenau equation using an analytical method
- Computational examination of Jeffrey nanofluid through a stretchable surface employing Tiwari and Das model
- Numerical analysis of a single-mode microring resonator on a YAG-on-insulator
- Review Articles
- Double-layer coating using MHD flow of third-grade fluid with Hall current and heat source/sink
- Analysis of aeromagnetic filtering techniques in locating the primary target in sedimentary terrain: A review
- Rapid Communications
- Nonlinear fitting of multi-compartmental data using Hooke and Jeeves direct search method
- Effect of buried depth on thermal performance of a vertical U-tube underground heat exchanger
- Knocking characteristics of a high pressure direct injection natural gas engine operating in stratified combustion mode
- What dominates heat transfer performance of a double-pipe heat exchanger
- Special Issue on Future challenges of advanced computational modeling on nonlinear physical phenomena - Part II
- Lump, lump-one stripe, multiwave and breather solutions for the Hunter–Saxton equation
- New quantum integral inequalities for some new classes of generalized ψ-convex functions and their scope in physical systems
- Computational fluid dynamic simulations and heat transfer characteristic comparisons of various arc-baffled channels
- Gaussian radial basis functions method for linear and nonlinear convection–diffusion models in physical phenomena
- Investigation of interactional phenomena and multi wave solutions of the quantum hydrodynamic Zakharov–Kuznetsov model
- On the optical solutions to nonlinear Schrödinger equation with second-order spatiotemporal dispersion
- Analysis of couple stress fluid flow with variable viscosity using two homotopy-based methods
- Quantum estimates in two variable forms for Simpson-type inequalities considering generalized Ψ-convex functions with applications
- Series solution to fractional contact problem using Caputo’s derivative
- Solitary wave solutions of the ionic currents along microtubule dynamical equations via analytical mathematical method
- Thermo-viscoelastic orthotropic constraint cylindrical cavity with variable thermal properties heated by laser pulse via the MGT thermoelasticity model
- Theoretical and experimental clues to a flux of Doppler transformation energies during processes with energy conservation
- On solitons: Propagation of shallow water waves for the fifth-order KdV hierarchy integrable equation
- Special Issue on Transport phenomena and thermal analysis in micro/nano-scale structure surfaces - Part II
- Numerical study on heat transfer and flow characteristics of nanofluids in a circular tube with trapezoid ribs
- Experimental and numerical study of heat transfer and flow characteristics with different placement of the multi-deck display cabinet in supermarket
- Thermal-hydraulic performance prediction of two new heat exchangers using RBF based on different DOE
- Diesel engine waste heat recovery system comprehensive optimization based on system and heat exchanger simulation
- Load forecasting of refrigerated display cabinet based on CEEMD–IPSO–LSTM combined model
- Investigation on subcooled flow boiling heat transfer characteristics in ICE-like conditions
- Research on materials of solar selective absorption coating based on the first principle
- Experimental study on enhancement characteristics of steam/nitrogen condensation inside horizontal multi-start helical channels
- Special Issue on Novel Numerical and Analytical Techniques for Fractional Nonlinear Schrodinger Type - Part I
- Numerical exploration of thin film flow of MHD pseudo-plastic fluid in fractional space: Utilization of fractional calculus approach
- A Haar wavelet-based scheme for finding the control parameter in nonlinear inverse heat conduction equation
- Stable novel and accurate solitary wave solutions of an integrable equation: Qiao model
- Novel soliton solutions to the Atangana–Baleanu fractional system of equations for the ISALWs
- On the oscillation of nonlinear delay differential equations and their applications
- Abundant stable novel solutions of fractional-order epidemic model along with saturated treatment and disease transmission
- Fully Legendre spectral collocation technique for stochastic heat equations
- Special Issue on 5th International Conference on Mechanics, Mathematics and Applied Physics (2021)
- Residual service life of erbium-modified AM50 magnesium alloy under corrosion and stress environment
- Special Issue on Advanced Topics on the Modelling and Assessment of Complicated Physical Phenomena - Part I
- Diverse wave propagation in shallow water waves with the Kadomtsev–Petviashvili–Benjamin–Bona–Mahony and Benney–Luke integrable models
- Intensification of thermal stratification on dissipative chemically heating fluid with cross-diffusion and magnetic field over a wedge