Tomography workshop Samuli Siltanen Department of Mathematics and - - PowerPoint PPT Presentation

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Tomography workshop Samuli Siltanen Department of Mathematics and - - PowerPoint PPT Presentation

Tomography workshop Samuli Siltanen Department of Mathematics and Statistics University of Helsinki, Finland samuli.siltanen@helsinki.fi www.siltanen-research.net Summer school University of Helsinki Kumpula Campus, June 1012, 2019 Lotus


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SLIDE 1

Tomography workshop

Samuli Siltanen

Department of Mathematics and Statistics University of Helsinki, Finland samuli.siltanen@helsinki.fi www.siltanen-research.net

Summer school University of Helsinki Kumpula Campus, June 10–12, 2019

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SLIDE 2

Lotus root tomography

YouTube search: “lotus tomography” www.youtube.com/watch?v=eWwD_EZuzBI&t=7s Video: thanks to Tatiana Bubba, Andreas Hauptmann and Juho Rimpeläinen

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SLIDE 3

Outline

X-ray attenuation as line integral Construction of the sinogram

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SLIDE 4
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SLIDE 5
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SLIDE 6

X-ray intensity attenuates inside matter, here shown with a homogeneous block

https://www.youtube.com/watch?v=IfXo2S1xXCQ

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SLIDE 7

Formula for X-ray attenuation along a line inside homogeneous matter

An X-ray with intensity I0 enters a homogeneous physical body.

I0 I1

  • s

The intensity I1 of the X-ray when it exits the material is

I1 = I0e−µs,

where s is the length of the path of the X-ray inside the body and µ > 0 is X-ray attenuation coefficient.

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SLIDE 8

X-ray intensity attenuates inside matter, here shown with two homogeneous blocks

https://www.youtube.com/watch?v=Z_IBFQcn0l8

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SLIDE 9

A digital X-ray detector counts how many photons arrive at each pixel

X-ray source

1000

photon count

1000

Detector

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SLIDE 10

Adding material between the source and detector reveals the exponential X-ray attenuation law

1000 1000 1000

photon count

1000 500 250

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SLIDE 11

We take logarithm of the photon counts to compensate for the exponential attenuation law

log

6.9 6.2 5.5

1000 1000 1000

photon count

1000 500 250

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SLIDE 12

Final calibration step is to subtract the logarithms from the empty space value (here 6.9)

log

6.9 6.2 5.5

1000 1000 1000

photon count

1000 500 250

line integral

0.0 0.7 1.4

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SLIDE 13

Formula for X-ray attenuation along a line: Beer-Lambert law

Let f : [a, b] → R be a nonnegative function modelling X-ray attenuation along a line inside a physical body. Beer-Lambert law connects the initial and final intensities: I1 = I0e−

b

a f (x)dx.

We can also write it in the form

− log(I1/I0) = b

a

f (x)dx,

where I0 is known from calibration and I1 from measurement.

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SLIDE 14

FIPS Computational Blog

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SLIDE 15

Outline

X-ray attenuation as line integral Construction of the sinogram

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SLIDE 16

Construction of the sinogram

Angle of X-rays: 3.0 degrees

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SLIDE 17

Construction of the sinogram

Angle of X-rays: 12.2 degrees

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SLIDE 18

Construction of the sinogram

Angle of X-rays: 21.5 degrees

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SLIDE 19

Construction of the sinogram

Angle of X-rays: 30.7 degrees

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SLIDE 20

Construction of the sinogram

Angle of X-rays: 39.9 degrees

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SLIDE 21

Construction of the sinogram

Angle of X-rays: 49.2 degrees

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SLIDE 22

Construction of the sinogram

Angle of X-rays: 58.4 degrees

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SLIDE 23

Construction of the sinogram

Angle of X-rays: 67.6 degrees

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SLIDE 24

Construction of the sinogram

Angle of X-rays: 76.8 degrees

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SLIDE 25

Construction of the sinogram

Angle of X-rays: 86.1 degrees

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SLIDE 26

Construction of the sinogram

Angle of X-rays: 95.3 degrees

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SLIDE 27

Construction of the sinogram

Angle of X-rays: 104.5 degrees

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SLIDE 28

Construction of the sinogram

Angle of X-rays: 113.8 degrees

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SLIDE 29

Construction of the sinogram

Angle of X-rays: 123.0 degrees

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SLIDE 30

Construction of the sinogram

Angle of X-rays: 132.2 degrees

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SLIDE 31

Construction of the sinogram

Angle of X-rays: 141.5 degrees

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SLIDE 32

Construction of the sinogram

Angle of X-rays: 150.7 degrees

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SLIDE 33

Construction of the sinogram

Angle of X-rays: 159.9 degrees

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SLIDE 34

Construction of the sinogram

Angle of X-rays: 169.2 degrees

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SLIDE 35

Construction of the sinogram

Angle of X-rays: 178.4 degrees

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SLIDE 36

Construction of the sinogram

Angle of X-rays: 187.6 degrees

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SLIDE 37

Construction of the sinogram

Angle of X-rays: 196.8 degrees

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SLIDE 38

Construction of the sinogram

Angle of X-rays: 206.1 degrees

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SLIDE 39

Construction of the sinogram

Angle of X-rays: 215.3 degrees

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SLIDE 40

Construction of the sinogram

Angle of X-rays: 224.5 degrees

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SLIDE 41

Construction of the sinogram

Angle of X-rays: 233.8 degrees

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SLIDE 42

Construction of the sinogram

Angle of X-rays: 243.0 degrees

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SLIDE 43

Construction of the sinogram

Angle of X-rays: 252.2 degrees

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SLIDE 44

Construction of the sinogram

Angle of X-rays: 261.5 degrees

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SLIDE 45

Construction of the sinogram

Angle of X-rays: 270.7 degrees

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SLIDE 46

Construction of the sinogram

Angle of X-rays: 279.9 degrees

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SLIDE 47

Construction of the sinogram

Angle of X-rays: 289.2 degrees

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SLIDE 48

Construction of the sinogram

Angle of X-rays: 298.4 degrees

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SLIDE 49

Construction of the sinogram

Angle of X-rays: 307.6 degrees

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SLIDE 50

Construction of the sinogram

Angle of X-rays: 316.8 degrees

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SLIDE 51

Construction of the sinogram

Angle of X-rays: 326.1 degrees

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SLIDE 52

Construction of the sinogram

Angle of X-rays: 335.3 degrees

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SLIDE 53

Construction of the sinogram

Angle of X-rays: 344.5 degrees

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SLIDE 54

Construction of the sinogram

Angle of X-rays: 353.8 degrees

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SLIDE 55

We have object and data for the inverse problem

  • A

f ∈ R32×32 Af ∈ R49×39

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SLIDE 56

Illustration of the ill-posedness of tomography

Difference 0.02672

  • A

A

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SLIDE 57

Illustration of the ill-posedness of tomography

Difference 0.00899

  • A

A

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SLIDE 58

Illustration of the ill-posedness of tomography

Difference 0.00254

  • A

A

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SLIDE 59

Illustration of the ill-posedness of tomography

Difference 0.00124

  • A

A

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SLIDE 60

Illustration of the ill-posedness of tomography

Difference 0.00004

  • A

A