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MR-DTI:Non-invasive imaging of neuroanatomy of white matter
Guido Gerig
Slide 2
Acknowledgments
Contributors:
• Martin Styner • Susumu Mori• Andy Alexander• Gordon Kindlmann• Randy Gollub
• National Alliance for Medical Image Computing (NIH U54EB005149)
Slide 3
Use of these slides
• Slides were borrowed from various researchers, and we are working on getting permissions for distribution.
• Slides can be used for own purposes. • Please do not distribute these slides. • Please do no put slides into public download
space.
T1w T2w
Slide 5
Slide 6
5D 6Mo 14Mo
Slide 7
Networking and Brain Connectivity
Major Fiber Tracts extracted from DT MRI
UNC Computer Science: Network wire cabinets
Slide 8Diffusion Tensor Imaging (DT MRI) reveals
White Matter Structure
Gray matter
White matter
Courtesy of Susumu Mori, JHU
DT MRI
Slide 9
White Matter Structure
• Goal: Measure properties associated with the directiondirection of white matter Fibers
White matter
Wh
ite M
atte
rF
ibe
rs
Slide 10
Example: Corticospinal Tract
Tractography: Coronal viewTractography: Coronal view
Source: Duke NeuroAnatomy Web Resources (Christine Hulette)
B: Superior longitudinal fasciculus
C: Superior occipitofrontal fasciculus
D: Cingulum
E: Inferior longitudinal fasciculus
F: Inferior occipitofrontal fasciculus
Slide 11
Diffusion
• Random ‘Walk’ of Water Molecules
1 2 3
x2 6D
DT-MRI A. Alexander
Slide 12
Diffusion• Diffusion: Brownian motion of one material
through another
• Anisotropy: diffusion rate depends on direction
Gordon Kindlimann
Kleenex newspaper
Slide 13
Biological Restricted Diffusion
• Sextra >> Sintra
• Diffusion influenced by mean free path– Tortuosity
DT-MRI A. Alexander
Slide 14
Biological Restricted Diffusion
• Cellular degeneration (necrosis)- Diffusion increases
DT-MRI A. Alexander
Slide 15
Aniostropic Restricted Diffusion
• Diffusion has angular dependence
DT-MRI A. Alexander
How can we measure diffusion without perturbing the system?
Slide 17
Slide 18
Diffusion and white matter• Diffusion MRI measures diffusion of mainly water
molecules – Isotropic medium → molecules move with Brownian motion.– In biological tissues diffusion is often anisotropic
• In white matter: “Local structure”– Insulating myelin sheet, low probability to cross into axon– Dense axon bundles exhibits strongly directional local structure– Diffusion along fiber bundle is main diffusion direction
Myelin sheet Nodes of Ranvier
Main diffusion direction
Slide 19
(An)isotropic diffusion
Free diffusion
Restricted diffusion
Isotropic diffusion
Anisotropic diffusion
Courtesy of Susumu Mori, John Hopkins University Medical School
Probability Distribution
Probability Distribution
Slide 20
DWI (indirectly) senses the structure of the tissue by measuring water molecule
displacement along a chosen direction.
r
r'
y
diffusioncoefficientin the y direction(= Dy)
Start
End
Slide 21
r
r'
If the path of the water molecule is affected by restrictions such as cellular material, the measured diffusion coefficient is reduced
extracellularspace
intracellularspace
Slide 22
If the tissue structures are oriented, the path of the water molecule (and the measured diffusion coefficients) will reflect this.
r
r'
y
diffusioncoefficientin the y direction(= Dy)
x diffusion coefficientin the x direction(= Dx)
Dx > Dy
Magnetic Resonance Imaging (MRI)
• Larmor Frequency
• Magnetic Field Gradient, G
Diffusion Weighted (DW) MRI
• Accumulated Phase
)t(G
DW-MRI II
x
N
ox Attenuation!
Slide 26
The pixel signal intensity, S, is related to the b-value and the diffusion coefficient, D, through:
This equation (Steyskal Tanner Equation) has two unknowns, the signal intensity for b = 0
(S0) and D. Therefore, at least 2 measurements must be made, each at a
different b-value to calculate D.
DbeSS
0
Equation for the diffusion attenuation
GG
b-value
Sig
nal I
nten
sity
D
lnSS0
2G2 2
3
D= - bD
Slide 28
Measuring D for a Given Direction: Simplified model of two b values
(b=0 and b=nnnn)
b-value
ln(S)
slope = D
intercept = S0
0 1000
DWI and ADC
1 G/cm 6 G/cm 10 G/cm 13 G/cm
b-value
Sig
nal I
nten
sity
Slide 30
The b-value is the contrast “knob” in a diffusion experiment and is varied in magnitude and in a
specified number of directions.
Increasing the b-value increases the contrast between slow and fast diffusing water molecules.
Increasing b-value
Images courtesy: Susumu Mori (JHU)
Slide 31
Apparent Diffusion Coefficient (ADC) Map with Different Measurement Direction
YX ZOnly the diffusion along a gradient direction can be measured
Courtesy of Susumu Mori, John Hopkins University Medical School
Gradient direction
ASNR 2003 –Washington,DC DT-MRI Alexander
Diffusion Weighted Images
12 DW encoding directionsSi (b=912 sec/mm2)
T2W ReferenceSo (b ~ 0 sec/mm2)
)ˆˆexp( itioi ggbSS D
)3/(222 Gb
Courtesy JE Lee
Slide 33
Measurement along Multiple Directions
Modified from DavidTuch, MGH
• Diffusion MRI measures along single gradient directions– Diffusion Weighted Images (DWI)
• In principle: Arbitrary gradient directions• 6 different directions → Tensor
– 12/24 directions → stability– Diffusion Tensor Imaging (DTI)
• High angular acquisition– Sampling of orientation diffusion– Higher order representations (fiber crossings)– Qball (D. Tuch, MGH), >256 dirs– Others: Van Wedeen (MIT), Frank (UCSD)
Slide 34
DWI: Three Coordinate Systems
rightanterior
supe
riorWorld:
e.g. “RAS”
fast=I
med
ium
=J
slow=KImage:“IJK” Gradients:
g1 = (1,0,1)g2 = (1,-1,0)… Dxx, Dxy …
x
y
z
“ImageOrientation”
“MeasurementFrame”
ASNR 2003 –Washington,DC DT-MRI Alexander
Measured Apparent Diffusivities
12 encoding directions
b
SSD ioi
lnln
Courtesy JE Lee
Slide 36
What is “Diffusion – Weighted” Imaging?
In “Conventional” MRI, image contrast reflectsthe local relaxation (T1, T2) environment of the water molecules.
In “Diffusion-Weighted” Imaging (DWI), imagecontrast reflects the physical structure of the Tissue (via the local diffusion distribution).
Slide 37
Simplification and assumption
Diffusion ellipsoidCourtesy of Susumu Mori, John Hopkins University Medical School
Orientational Diffusion Fct
ASNR 2003 –Washington,DC DT-MRI Alexander
The Diffusion Tensor
zzzyzx
yzyyyx
xzxyxx
DDD
DDD
DDD
D
0,, zzyyxx DDD zyyzzxxzyxxy DDDDDD ;;
Courtesy JE Lee
National Alliance for Medical Image Computing http://na-mic.org
DWI summary: MRI
• Diffusion: Brownian motion of one material through another
• Anisotropy: diffusion rate depends on direction
• Magnetic gradients create spatial planar waves of proton phase
• Destructive interference measures diffusion along gradient direction only
Kleenex newspaper
National Alliance for Medical Image Computing http://na-mic.org
DWI crash course: Model
Single Tensor Model (Basser 1994)
A0
gi
Ai
D
Dxx Dxy Dxz
Dyy Dyz
Dzz
Tensorestimation
Slide 41
Anisotropy & Color-coded Orientation
Isotropic GM
Anisotropic WM
Courtesy of Susumu Mori, John Hopkins University Medical School
Slide 42
DTI Tensor Visualization
Color: FA valueITK: DTIFiberTubeSpatialObject & SpatialObjectViewers (Julien Jomier)
Here comes Ross Whitaker