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Data Acquisition, Representation and Reconstruction of medical images

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Title: Data Acquisition, Representation and Reconstruction of medical images


1
Data Acquisition, Representation and
Reconstruction of medical images
Application of Advanced Spectral Methods
2
Acquisition Methods for medical images
  • X-Rays
  • Computer Tomography (CT or CAT)
  • MRI (or NMR)
  • PET / SPECT (Positron Emission Tomography,
    Single Photon Emission Computerized Tomography
  • Ultrasound
  • Computational

3
X-Rays
4
X-Rays - Physics
  • X-Rays are associated with inner shell electrons
  • As the electrons decelerate in the target through
    interaction, they emit electromagnetic radiation
    in the form of x-rays.
  • patient is located between an x-ray source and a
    film -gt radiograph
  • cheap and relatively easy to use
  • potentially damaging to biological tissue

5
X-Rays
  • X-Rays
  • similar to visible light, but higher energy!

6
X-Rays - Visibility
  • bones contain heavy atoms -gt with many electrons,
    which act as an absorber of x-rays
  • commonly used to image gross bone structure and
    lungs
  • excellent for detecting foreign metal objects
  • main disadvantage -gt lack of anatomical structure
  • all other tissue has very similar absorption
    coefficient for x-rays

7
X-Rays - Images
X-Rays can be used in computerized tomography
8
  • Computerized (Axial) Tomography

9
CT (CAT) scanners and relevant mathematics
10
Non-Intrusive Medical Diagnosis based on
Computerized Tomography
  • Computer tomography CT

(From Jains Fig.10.1)
An X-ray CT scanning system
11
Non-Intrusive Medical Diagnosis based on
Transmission Tomography
Source and Detector are rotating around humans
body
(From Boviks Handbook Fig.10.2.1)
12
Non-Intrusive Medical Diagnosis based on
projections
  • Observe a set of projections (integrations) along
    different angles of a cross-section
  • Each projection itself loses the resolution of
    inner structure
  • Types of measurements
  • transmission (X-ray),
  • emission, magnetic resonance (MRI)
  • Want to recover inner structure from the
    projections
  • Computerized Tomography (CT)

13
Non-Intrusive Medical Diagnosis based on Emission
Tomography
  • Emission tomography ET measure emitted gamma
    rays by the decay of isotopes from radioactive
    nuclei of certain chemical compounds affixed to
    body parts.
  • MRI based on that protons possess a magnetic
    moment and spin.
  • In magnetic field gt align to parallel or
    antiparallel.
  • Apply RF gt align to antiparallel. Remove RF gt
    absorbed energy is remitted and detected by
    Rfdetector.

f(x,y) is 2D image as before
14
Radon Transform Principles
  • A linear transform f(x,y) ? g(s,?)
  • Line integral or ray-sum
  • Along a line inclined at angle ? from y-axis and
    s away from origin
  • Fix ? to get a 1-D signal g?(s)

We have now a set of images g?(s) which represent
g(s,?)
(From Jains Fig.10.2)
This is a transform from 2D to 2D spaces
15
Tomography and Reconstruction
  • Lecture Overview
  • Applications
  • Background/history of tomography
  • Radon Transform
  • Fourier Slice Theorem
  • Filtered Back Projection
  • Algebraic techniques
  • Measurement of Projection data
  • Example of flame tomography

16
Applications Types of Tomography
MRI and PET showing lesions in the brain.
PET scan on the brain showing Parkinsons Disease
17
Applications Types of Tomography non medical
ECT on industrial pipe flows
18
CT or CAT - Principles
  • Computerized (Axial) Tomography
  • introduced in 1972 by Hounsfield and Cormack
  • natural progression from X-rays
  • based on the principle that a three-dimensional
    object can be reconstructed from its two
    dimensional projections
  • based on the Radon transform (a map from an
    n-dimensional space to an (n-1)-dimensional space)

Radon again!
From 2D to 3D !
19
CT or CAT - Methods
  • measures the attenuation of X-rays from many
    different angles
  • a computer reconstructs the organ under study in
    a series of cross sections or planes
  • combine X-ray pictures from various angles to
    reconstruct 3D structures

20
The History of CAT
  • Johan Radon (1917) showed how a reconstruction
    from projections was possible.
  • Cormack (1963,1964) introduced Fourier
    transforms into the reconstruction algorithms.
  • Hounsfield (1972) invented the X-ray Computer
    scanner for medical work, (which Cormack and
    Hounsfield shared a Nobel prize).
  • EMI Ltd (1971) announced development of the EMI
    scanner which combined X-ray measurements and
    sophisticated algorithms solved by digital
    computers.

21
  • Backpropagation
  • Principles

22
Backpropagation
We know that objects are somewhere here in black
stripes, but where?
23
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24
Example of Simple Backprojection Reconstruction
  • Given are sums, we have to reconstruct values of
    pixels A, B, C and D

25
Image Reconstruction ART or Algebraic
Reconstruction Technique
ART
26
CT - Reconstruction ART or Algebraic
Reconstruction Technique
  • METHOD 1 Algebraic Reconstruction Technique
  • iterative technique
  • attributed to Gordon

Initial Guess
Reconstructedmodel
Back-Projection
Projection
Actual DataSlices
27
CT - Reconstruction FBP Filtered Back Propagation
  • METHOD 2 Filtered Back Projection
  • common method
  • uses Radon transform and Fourier Slice Theorem

y
F(u,v)
f(x,y)
Gf(r)
x
s
u
gf(s)
f
Spatial Domain
Frequency Domain
28
COMPARISON CT - FBP vs. ART
ART
FBP
Algebraic Reconstruction Technique
  • Still slow
  • better quality for fewer projections
  • better quality for non-uniform project.
  • guided reconstruct. (initial guess!)

Filtered Back Projection
  • Computationally cheap
  • Clinically usually 500 projections per slice
  • problematic for noisy projections

29
  • Fourier Slice Theorem and FFT review

Patients body is described by spatial
distribution of attenuation coefficient
30
Properties of attenuation coefficient
Our transform f(x,y) ? p(r,?)
31
  • attenuation coefficient is used in CT_number of
    various tissues
  • These numbers are represented in HU Hounsfield
    Units

CT_number uses attenuation coefficients
32
RADON TRANSFORM Properties
REMEMBER f(x,y) ? p(r,?)
33
Radon Transform is available in Matlab
  • Radon and its inverse easy to use
  • You can do your own projects with CT
    reconstruction
  • Data are available on internet

sinogram
34
Inverse Radon Transform
Inverse Radon Transform
35
  • Matlab examples

36
Sinogram versus Hough
37
An aside
The object
The sinogram
  • AN ASIDE

38
Review and notation Fourier Transform of Image
f(x,y)
39
Matlab example
In Matlab there are implemented functions that
use Fourier Slice Theorem
40
Matlab example filtering
High frequency removed
Low frequency removed
41
Matlab example - convolution
42
Remainder of main theorem of spectral imaging
Matlab example filtering by convolution in
spectral domain
43
  • Radon Transform and a Head Phantom

44
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45
Reconstructing with more and more rays
46
Example of Image Radon Transform
Y-axis distance, X-axis angle
(From Matlab Image Processing Toolbox
Documentation)
47
  • Matlab Implementation of Radon Transform

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50
big noise
No noise
51
The Lung Cancer and the reconstruction
52
The Lung and The CTs
LUNG 1.Either of the pair of organs occupying
the cavity of the thorax that effect the aeration
of the blood. 2.Balloon-like structures in the
chest that bring oxygen into the body and expel
carbon dioxide from the body
TYPES 1.Small Cell Lung Cancer (SCLC) - 20 of
all lung cancers 2.Non Small Cell Lung Cancer
(NSCLC) - 80 of all lung cancer
Risks In the United States alone, it is
estimated that 154,900 died from lung cancer in
2002. In comparison,is estimated that 126,800
people died from colon, breast and prostate
cancer combined, in 2002.
LUNG CANCER Lung Cancer happens when cells in
the lung begin to grow out of control and can
than invade nearby tissues or spread throughout
the body Large collections of this out of
control tissues are called tumors.
53
Starting Point
We want to reconstruct shape of the lungs
Border Detection
  • At the moment two approaches are available.
  • Left the algorithm developed at Pisa
  • Right the algorithm developed at Lecce

54
Image Interpolation - Theory
IDEA In order to provide a richer environment
we are thinking of using interpolation methods
that will generate artificial images thus
revealing hidden information.
RADON RECONSTRUCTION Radon reconstruction is
the technique in which the object is
reconstructed from its projections. This
reconstruction method is based on approximating
the inverse Radon Transform.
RADON Transform The 2-D Radon transform is the
mathematical relationship which maps the spatial
domain (x,y) to the Radon domain (p,phi). The
Radon transform consists of taking a line
integral along a line (ray) which passes through
the object space. The radon transform is
expressed mathematically as
FILTERED BACK PROJECTION - INVERSE R.T. It is
an approximation of the Inverse Radon
Transform. The principle Several x-ray images
of a real-world volume are acquired The Data
X-ray images (projections) of known orientation,
given by data samples. The Goal Reconstruct a
numeric representation of the volume from these
samples. The Mean Obtain each voxel value from
its pooled trace on the several
projections. Resampling At this point one can
obtain the artificial slices Reslicing An
advantage of the volume reconstruction is the
capability of obtaining new perpendicular slices
on the original ones.
55
Image Interpolation - Graphical Representation (I)
56
Image Interpolation - Graphical Representation
(II)
57
Line Integrals and Projections
  • We review the principle
  • Discuss various geometries
  • Show the use of filtering

58
Line Integrals and Projections
59
Fan Beams
Parallel Beams
A fan beam projection is taken if the rays meet
in one location
Parallel beams projections are taken by measuring
a set of parallel rays for a number of different
angles
Various types of beams can be used
60
Line Integrals and Projections
A projection is formed by combining a set of line
integrals. Here the simplest projection, a
collection of parallel ray integrals i.e constant
?, is shown.
Notation for calculations in these projections
61
Line Integrals and Projections
A simple diagram showing the fan beam projection
62
Fourier Slice Theorem
63
Fourier Slice Theorem
  • The Fourier slice theorem is derived by taking
    the one-dimensional Fourier transform of a
    parallel projection and noting that it is equal
    to a slice of the two-dimensional Fourier
    transform of the original object.
  • It follows that given the projection data, it
    should then be possible to estimate the object by
    simply performing the 2D inverse Fourier
    transform.

Start by defining the 2D Fourier transform of the
object function as
For simplicity ?0 which leads to v0
  • Define the projection at angle ? P?(t)
  • Define its transform by

As the phase factor is no-longer dependent on y,
the integral can be split.
64
Fourier Slice Theorem
As the phase factor is no-longer dependent on y,
the integral can be split.
The part in brackets is the equation for a
projection along lines of constant x
Substituting in
Thus the following relationship between the
vertical projection and the 2D transform of the
object function
65
Fourier Slice Theorem Stanley and Kak
  • Full details of derivation, not for now.

66
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67
The Fourier Slice Theorem
The Fourier Slice theorem relates the Fourier
transform of the object along a radial line.
t
Fourier transform
?
Space Domain
Frequency Domain
68
The Fourier Slice Theorem
The Fourier Slice theorem relates the Fourier
transform of the object along a radial line.
Collection of projections of an object at a
number of angles
t
Fourier transform
?
  • For the reconstruction to be made it is common
    to determine the values onto a square grid by
    linear interpolation from the radial points.
  • But for high frequencies the points are further
    apart resulting in image degradation.

Space Domain
Frequency Domain
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71
Backprojection of Radon Transform
72
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75
Backprojection of Radon Transform
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77
Ideal cylinder
Blurred edges
Crisp edges
Filtered backpropagation creates crisp edges
78
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79
Computerized Tomography Equipment
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81
CT - 2D vs. 3D
  • Linear advancement (slice by slice)
  • typical method
  • tumor might fall between cracks
  • takes long time
  • helical movement
  • 5-8 times faster
  • A whole set of trade-offs

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84
Evolution of CT technology
85
CT or CAT - Advantages
  • significantly more data is collected
  • superior to single X-ray scans
  • far easier to separate soft tissues other than
    bone from one another (e.g. liver, kidney)
  • data exist in digital form -gt can be analyzed
    quantitatively
  • adds enormously to the diagnostic information
  • used in many large hospitals and medical centers
    throughout the world

86
CT or CAT - Disadvantages
  • significantly more data is collected
  • soft tissue X-ray absorption still relatively
    similar
  • still a health risk
  • MRI is used for a detailed imaging of anatomy
    no Xrays involved.

87
  • Nuclear Magnetic Resonance (NMR)
  • Magnetic Resonance Imaging (MRI)

88
MRI
  • Nuclear Magnetic Resonance (NMR) (or Magnetic
    Resonance Imaging - MRI)
  • most detailed anatomical information
  • high-energy radiation is not used, i.e. this is
    safe method
  • based on the principle of nuclear resonance
  • (medicine) uses resonance properties of protons

89
Magnetic Resonance ImagingMRI - polarized
  • all atoms (core) with an odd number of protons
    have a spin, which leads to a magnetic behavior
  • Hydrogen (H) - very common in human body very
    well magnetizing
  • Stimulate to form a macroscopically measurable
    magnetic field

90
MRI - Signal to Noise Ratio
  • proton density pictures - measures HMRI is good
    for tissues, but not for bone
  • signal recorded in Frequency domain!!
  • Noise - the more protons per volume unit, the
    more accurate the measurements - better signal to
    noise ratio (SNR) through decreased resolution

91
PET/SPECT
  • Positron Emission TomographySingle Photon
    Emission Computerized Tomography

92
PET/SPECT
  • Positron Emission TomographySingle Photon
    Emission Computerized Tomography
  • recent technique
  • involves the emission of particles of antimatter
    by compounds injected into the body being scanned
  • follow the movements of the injected compound and
    its metabolism
  • reconstruction techniques similar to CT - Filter
    Back Projection iterative schemes

93
Ultrasound
94
Ultrasound
  • the use of high-frequency sound (ultrasonic)
    waves to produce images of structures within the
    human body
  • above the range of sound audible to humans
    (typically above 1MHz)
  • piezoelectric crystal creates sound waves
  • aimed at a specific area of the body
  • change in tissue density reflects waves
  • echoes are recorded

95
Ultrasound (2)
  • Delay of reflected signal and amplitude
    determines the position of the tissue
  • still images or a moving picture of the inside of
    the body
  • there are no known examples of tissue damage from
    conventional ultrasound imaging
  • commonly used to examine fetuses in utero in
    order to ascertain size, position, or
    abnormalities
  • also for heart, liver, kidneys, gallbladder,
    breast, eye, and major blood vessels

96
Ultrasound (3)
  • by far least expensive
  • very safe
  • very noisy
  • 1D, 2D, 3D scanners
  • irregular sampling - reconstruction problems

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Typical Homework
101
Sources of slides and information
  • Badri Roysam
  • Jian Huang,
  • Machiraju,
  • Torsten Moeller,
  • Han-Wei Shen
  • Kai Thomenius
  • Badri Roysam
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