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Analysis of radiation transport in biological tissues using a deterministic code, partisin 4.0

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ANALYSIS OF RADIATION

TRANSPORT IN BIOLOGICAL TISSUES USING A DETERMINISTIC CODE,

PARTISIN 4.0

ANALYSIS OF RADIATION

TRANSPORT IN BIOLOGICAL TISSUES USING A DETERMINISTIC CODE,

PARTISIN 4.0

Murat AYDIN

Murat AYDIN

Nuclear Research Section

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General Objective of Tomography

General Objective of Tomography

Constructing the image

to diagnose

inhomogeneties or morphological changes

(3)

What is optical tomograhy?

Optical tomograhy is a form of computed tomograhy that creates a digital volumetric model of an object by

reconstructing images made from light transmitted and scattered through an object

(4)

Optical Tomography

Optical Tomography

• AdvantagesAdvantages

• Reduction of invasiveness Reduction of invasiveness

• Better treatments at reduced costBetter treatments at reduced cost • Inexpensive and portable systemInexpensive and portable system

(5)

Why NIR Photons?

Why NIR Photons?

 NIR Wavelength 600-1300 nm NIR Wavelength 600-1300 nm

Absorption coefficient 0.001 – 0.01 mm-1Absorption coefficient 0.001 – 0.01 mm-1 Scattering coefficient 10 – 100 mm-1 Scattering coefficient 10 – 100 mm-1

UV

UV NLNL

NIR

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The Forward and Inverse

Photon Propagation Problem

The Forward and Inverse

Photon Propagation Problem

Forward problem:

Forward problem:

properties + source responses

properties + source responses

Inverse problem

Inverse problem

:

:

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Forward vs. inverse problem

Forward vs. inverse problem

Incident light and object optical properties Output light intensity

Knowing the cause Predict the effect  Forward problem (usually well-posed problem)

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Forward vs. inverse problem

Forward vs. inverse problem

 Inverse problem Inverse problem (usually ill-posed problem)(usually ill-posed problem)

Knowing the effect

Knowing the effect Predict the causePredict the cause

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PARTISN 4.0

PARTISN 4.0

 AA modular computer program package designed to solve modular computer program package designed to solve

the time-independent or dependent multigroup discrete

the time-independent or dependent multigroup discrete

ordinates form of the Boltzmann transport equation in

ordinates form of the Boltzmann transport equation in

several different geometries.

several different geometries.

 33 distinct modules: the Input Module distinct modules: the Input Module((inputinput processingprocessing)), ,

the Solver Module

the Solver Module((the transport equation solvingthe transport equation solving)), and , and the Edit Module

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Solution Methods

Solution Methods

The Solver Module contains one, two, and three-The Solver Module contains one, two, and

three-dimensional solvers in a single module.

dimensional solvers in a single module.

 In addition to the diamond-differencing method, the Solver In addition to the diamond-differencing method, the Solver

Module also has Adaptive Weighted Diamond-Differencing

Module also has Adaptive Weighted Diamond-Differencing

(AWDD), Linear Discontinuous (LD), and Exponential

(AWDD), Linear Discontinuous (LD), and Exponential

Discontinuous (ED) spatial differencing methods

(11)

Sample Forward Problems

(Problem 1)

Sample Forward Problems

(Problem 1)

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Optical Properties of Tissue

Like Media

Optical Properties of Tissue

Like Media

Material µs (cm–1 ) µ a (cm–1 ) 1 7 0.02 2 7.22 2.63 3 3.67 0.07

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Planes Passing Tthrough The

Medium

(14)

Scalar Fluency Rate Distribution Along the Planes (Problem 1)

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Angular Fluency Rate Distribution Along the Right Side of the Medium Angular Fluency Rate Distribution Along the Right Side of the Medium

(16)

Problem 2

Problem 2

(17)

Scalar Fluence Rate Distribution

Along the Planes for Problem 2

Scalar Fluence Rate Distribution

Along the Planes for Problem 2

(18)

Angular Fluence Rate Distribution Along

the Right Side of the Medium for Problem 2 Angular Fluence Rate Distribution Along

(19)

Comparison of Scalar Fluence Rates

at Detector Surface

Comparison of Scalar Fluence Rates

at Detector Surface

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 TThis his studystudy has aimed to review a deterministic has aimed to review a deterministic

code PARTISN for forward problems in

code PARTISN for forward problems in

scattering media such as biological tissue.

scattering media such as biological tissue.

 This is the first step to construct the images of This is the first step to construct the images of

biological tissues using near infrared light (NIR).

biological tissues using near infrared light (NIR).

 Next, Henyey–Greenstein scattering phase Next, Henyey–Greenstein scattering phase

function will be implemented into the code and,

function will be implemented into the code and,

inverse problem will be solved.inverse problem will be solved.

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