Lecture 18: Photon Dose Algorithms

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25 Terms

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Which algorithms are model based?

convolution superposition and MC and Boltzmann Transport solvers

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What are the major advances in dose algoritms?

  1. Splitting radiation dose into primary and secondary components

  2. Tissue densitometry using x-ray CT

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correction-based dose algoritms

corrects dose distribution in water under standard condition to that of the patient deliver, contour and heterogeneity

<p>corrects dose distribution in water under standard condition to that of the patient deliver, contour and heterogeneity</p>
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model-based dose algorithms

compute dose from first principle using patient geometry and density data and a model of radiation beam

<p>compute dose from first principle using patient geometry and density data and a model of radiation beam</p>
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What two effects should be considered for tissue inhomogeneties?

  1. attenuation of primary beam (distribution of scattered photons)

  2. secondary electron fluence

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Purpose of Ray tracing?

  1. Predict path of primary photons throughout patient volume

  2. Reshape kernels for each pair of interaction-dose deposition sites

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Most commonly used convolution based method

convolve impulse (TERMA at a point) function with energy deposition kernel

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Why is Terma commonly used for convolution based algoritms? Why no collisional Kerma?

Collisional kerma will underestimate the dose; it excludes radiative loss by charged particles

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How is Terma computed?

model fluence from linac head and transport it through the patient

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<p>If beam hardening is not being considered, what can be pulled out of the integral?</p>

If beam hardening is not being considered, what can be pulled out of the integral?

Ό/ρ

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What are the real-life complications of spatially invaraint kernels used in convolution-based photon dose algoritms?

tissue inhomogeneities, polyenergetic beams, beam divergence

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How are inhomogeneities dealt with in model-based dose calculations with point kernels?

  1. Model incident fluence as it exits Linac head

  2. Project fluence through CT data, compute TERMA at each point as a function of radiological pathlength, attenuating it by Ό/ρ

  3. Scale kernel as a function of radiological pathlength between interaction point and dose point

  4. Perform 3D convolution/ superposition

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O’Connor’s Theorem

O'Connor's scaling theorem says that the ratio of the fluence of secondary particles to that of primary particles, caused by an external source irradiating a medium in a collimated beam, is the same in two uniform media of the same composition but different density, provided geometrical distances are scaled inversely to density.

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Is Monte Carlo an approximation of the Boltzmann Equations?

No, it directly obtains the Boltzmann Transport Equations

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How are the boltzmann transport equations implemented clinically?

Linear Boltzmann Transport Equation solver with discrete ordinate approximation

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MC will converge if
.

infinite particles are used to run

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BTE will converge if


infinitesimally small energy, angle, and space grid sizes are used

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What limits the statical accuracy of MC algorithms?

number of histories run

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What limits quality of outcome for MC algorithms?

goodness of geometric model, tissue, and underlying physics data

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Why are MC algorithms used for MR-guided systems?

Can account for magnetic field

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What is a disadvantage of MC algorithms?

Long calculation times

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Is MC algorithms more common for electrons or photons?

electrons

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What so the BTE solution yield?

It yields the spatial distribution of charged particle fluences. This is converted to the dose distribution

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What is the speed of BTE dependent on?

dimensionality of problem

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How is electron contamination calculated?

scalar quantity added to the end