mipr lecture 7 copyright oleh tretiak, 2004 1 medical imaging and pattern recognition lecture 7...
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MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Medical Imaging and Pattern Recognition
Lecture 7 Computed Tomography
Oleh Tretiak
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Computer Tomography:How It Works
Only one plane is illuminated. Source-subject motion provides added information.
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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How it Works
• Original CT Scanner– Head only– One minute scanning time– Two sections– Ten minutes to compute images– Extremely successful!
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Contemporary Spiral Scanner
• Configuration:– 40 slices per rotation maximum
• Other options are 32 slices or 16 slices
– 40 mm axial distance scanned in one rotation
– 0.4 sec per rotation– 60 kW generator
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Example: Head
• Bleeding due to injury
• Can cause brain injury if not treated
• Blood between brain and dura, easy to treat
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Example: Head
• FRONTAL CONTUSION WITH SUBARACHNOID HEMORRHAGE
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Chest Study
• Pneumothorax (air between lung and chest)
• Also note the bilateral lower lobe consolidation of lungs, right being greater than left. There is a chest tube within the right hemithorax.
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Abdomen
• Appendicitis (arrow)
• Contrast agents in stomach and in blood
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Mathematics of Computed Tomography
• Model for measurements• Direct problem• Inverse problem• Algorithm for computed
tomography
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Direct Problem
• Beam with intensity I0 enters body with varying attenuation
• Each layer has thickness t
m m m mI I
m m m mI II I I
€
€
Ia = e−μ1tI0, Ib = e−μ 2tIa ,
Ic = e−μ 3tIb , I1 = e−μ 4 tIc
€
I1 = e−μ 4 te−μ 3te−μ 2te−μ1tI0 = e−(μ1 +μ 2 +μ 3 +μ 4 )tI0ln(I0 /I1) = (μ1 + μ2 + μ3 + μ4 )t
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Integral Equation
x
I (y)I
€
I1(y) = exp(− μ(x,y)dx∫ )I0
ln(I0 /I1(y)) = μ(x,y)dx∫
x
I (t, q)
I
y
q
t
€
ln(I0 /I1(t,θ)) = μ(t cosθ − lsinθ, t sinθ + lcosθ)dl∫
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Radon Transform
x
I (t, q)
I
y
q
t
f(x,y)
g(t, )
€
g(t,θ) = f (t cosθ − lsinθ, t sinθ + lcosθ)dl∫
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Inverse Radon Transform
• Given: X-ray transmission measurements I1(t, ). Find (x, y)
• Given: g(t, ). Find f(x, y)• Method:
– (a) convolution
– (b) backprojection
€
f (x,y) = g1(x cosθ + y sinθ,θ)dθ0
π
∫€
g1(t,θ) = h(t − τ )g(τ ,θ)dτ∫
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Example
-1
0
1
-1
0
1
-0.5
0
0.5
1
-1 -0.5 0 0.5 1
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
1
1.2
f(x, y)
Lines: g(t, ), same for all Dots: g1(t, ), after convolution
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Backprojection
-1
0
1
-1
0
1
-0.5
0
0.5
1
1.5
One, two, and four angles of backprojection
-1
0
1
-1
0
1
-0.5
0
0.5
1
1.5
-1
0
1
-1
0
1
-0.5
0
0.5
1
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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More Backprojection
-1
0
1
-1
0
1
-0.5
0
0.5
1
-1
0
1
-1
0
1
-0.5
0
0.5
1
-1
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1
-1
0
1
-0.5
0
0.5
1
8, 15, and 30 angle backprojection
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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History
• 1917, Joachim Radon– Solved formal inverse problem.
Interest in theory of integration and geometry
• 1958, Simeon Tetelbaum of KPI publishes a paper about X-ray tomography. – Publishes valid inverse problem
solution.
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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More History
• 1963 John Cormack publishes theoretical and experimental results.– Experiment with cylindrical objects
• 1972 Godfrey Hounsfield develops CT scanner
• 1979 Hounsfield and Cormack receive Nobel prize in Medicine
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Example of Contrast
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
12 bit image, full contrast range.
Window for lowdensities
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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More Contrast Operations
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Window for highdensities
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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3-D Images
• Spiral scan procedures produce sets of sectional images suitable for 3-D imaging
• Resectioning: Compute new section plane
• Projection: Compute sums along rays• Rendering: Segment image and show
surface.
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Medical Practice
• In the fall of 2003 Siemens became the first CT supplier ever to receive clearance from the FDA for a computer-aided technique of identifying nodules, that is, possible tumors, in the lung. CT is also used for the diagnosis of colon cancer: A virtual flight through the human colon can detect even the smallest polyps. If these are removed in time, an outbreak of colon cancer can very probably be prevented.
MIPR Lecture 7Copyright Oleh Tretiak, 2004
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Comparison
Left: A polyp seen with optical endoscopy. Right: View in virtual endoscopy.
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Summary
• Computer tomography became successful because it showed soft tissue differences that could not be seen on X-rays.
• Evolution of high-speed (spiral scan) machines came about through improvements in X-ray detectors
• This has led to 3-D imaging methods– Surgery planning– Virtual endoscopy