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Superresolution in MRI Imaging

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Title: Superresolution in MRI Imaging


1
Superresolution in MRI Imaging
  • Kenneth Neiss
  • April 15th, 2004

2
Introduction
  • Motivation
  • MRI Positive
  • Detects abnormalities in living tissue
  • Very good resolution in-plane
  • MRI Negative
  • Either
  • Does not provide high resolution in all
    dimensions (slice-select) with ample acquisition
    time
  • Acquires high resolution in all dimension (3-D)
    but requires much longer time to do so

3
MRI resolution dimensionality example
Courtesy of Greenspan et. al.
4
Introduction
  • What is needed?
  • Acquire high resolution images in all dimensions
  • Keep acquisition time relatively low
  • How to accomplish?
  • Apply techniques used in image sequence
    superresolution (CCD and video) to MR images

5
MRI Spatial Encoding
  • Background
  • Magnetic Resonance (MR)

6
MRI Mapping Process
7
Main Transforms in MRI
  • There are two main steps in the MRI process as
    detailed previously
  • the spin processing transform which encodes the
    data into the data space (k-space)
  • the data processing transform which converts the
    k-space data into a viewable image

8
Why are these steps important?
  • The data processing transform is considered the
    unarguable method for image reconstruction
  • The spin processing transform is the area by
    which the process has a direct affect on the
    ability for enhancing resolution by
    post-processing
  • Thus, this latter encoding step will be further
    studied

9
Spatial Encoding
  • Activated MR signal takes the form of a complex
    exponential thus, the encoding can be done
    with
  • Frequency encoding
  • Phase encoding

See paper for more details and descriptions
10
Properties of MRI Encoding
  • Signal is frequency encoded in one dimension
    in-plane and phase encoded in the other in-plane
    dimension
  • Upon application of gradients, a relationship
    between field strength and spatial location is
    identified
  • The atomic spins will resonate (precess) at
    frequencies singular to their location, allowing
    for reconstruction of 2-D or 3-D images
  • To fill the k-space (where the data is analyzed)
    requires N time-domain signals encoded with
    specific frequency and phase data to fill the NxN
    k-space

11
k-space analysis (see paper for derivations)
  • Frequency encoding gradient Gx maps a time signal
    to a k-space signal
  • Visible FT properties
  • As long as Gx ? 0, the frequency encoding
    gradient will uniquely encode the spatial
    information

12
k-space continued
  • When multiple gradients are used, the
    representation becomes in the form of a
    multidimensional FT, but S(k) is only present for
    a finite set of points for the k-space
  • k-space trajectory is a straight line dependent
    upon values of G (not straight line if G values
    not constant)
  • Phase encoding only affects the starting point of
    the trajectory and not the shape or form

13
Problems with 3D MRI
  • Acquiring 3-D voxels still might not provide the
    necessary resolution
  • Reducing the voxel size during acquisition
    actually decreases the SNR per voxel (shown
    through experiment that a decrease in voxel size
    in all dimensions of factor of 2 leads to
    decreased SNR by factor of 8)
  • Reducing voxel size leads to smaller volume
    coverage attainable without foldover effects
  • Applying a stronger magnetic field leads to
    higher motion artifacts and large distortions at
    the boundaries

14
2D MRI Slices
  • In cases where 3-D MRI is unattainable or
    undesirable, 2-D stacks of slices are produced
  • Problem does not yield best volume data when
    directly pieced together creates non-isotropic
    voxels with larger slice-select dimension than
    in-plane, resulting in higher resolution in-plane
    as compared with the slice-select dimension

Courtesy of Greenspan et. al.
15
Superresolution
  • Image sequence superresolution
  • Makes use of a set of degraded low resolution
    shifted versions of an image to create a higher
    resolution filtered image of the object
  • Interpolation first introduced by Tsai and Huang
  • Kim, Bose, and Valenzuela imposed the idea of
    using noisy and blurred low resolution images as
    the input to interpolate and sequentially filter
    in order to generate a high resolution filtered
    image
  • For simulation purposes, we need to reverse the
    process to extract a series of low resolution
    images to feed the system

16
Imaging System
Initial High Resolution Image Scheme
Resulting Low Resolution Image Set
Geometric Transform
Blur
Downsampling
Noise
Model of Near Field Imaging System
17
CCD and Video Image Characteristics
  • Images are not Fourier-encoded such as in MRI
    images
  • By overlaying various sub-pixel shifted versions
    of the object, one can extract extra Fourier data
    due to the shifts and piece together a higher
    resolution (in both in-plane dimensions)
    representation

18
MRI Image Characteristics
  • MRI data is acquired in 2-D stacks or 3-D slices
  • Data is inherently Fourier-encoded (frequency and
    phase)
  • The only new information that can be added with
    each successive slice or volume is the next piece
    in the stack (slice-select dimension)
  • This and the fact that the in-plane data is
    bandlimited lead to the idea that only the
    slice-select dimension can be utilized to improve
    resolution
  • Must take into account blurring by Point Spread
    Function (PSF)

19
Main Difference
  • Main difference between CCD/Video Camera Imaging
    and MRI Imaging
  • In Fourier-encoded 2-D MRI, there can be no
    additional information interpolated regarding
    high frequencies in the in-plane dimension only
    in the slice-select dimension can additional
    frequency information be extracted for 2-D MRI
    datasets
  • This is the basis for applying superresolution
    techniques in the slice-select direction for MRI
    images
  • In CCD and video camera imaging, superresolution
    can be applied to all dimensions (all dimensions
    can be used to extract high frequency data)
  • It has been shown that applying superresolution
    in MRI to the in-plane dimensions does not yield
    increased resolution and leads to similar results
    as if you zero-pad the temporal data shifting
    in-plane only provides a global phase shift in
    the time domain, not affecting the spatial
    frequency resolution

20
Additional Differences
  • Image registration
  • In MRI, registration is known beforehand (assume
    minimal subject motion) due to predetermined
    single time shift between slices (motion only in
    slice-select dimension)
  • MRI is similar to CCD, where there is a
    predetermined multisensor positioning resulting
    in subpixel shifts (all motion will occur
    in-plane, i.e. no panning, zooming, etc.)
  • Video Camera imaging has motion in all
    dimensions, and one must account for this using
    projective transformations
  • Since all of these imaging platforms have
    subpixel or subvoxel shifts, superresolution will
    be beneficial

21
Main MRI Tradeoff
  • Voxel Size vs. Acquisition Time
  • The smaller the isotropic voxel size, the longer
    the acquisition time (higher costs)
  • Solution
  • Implement a post-processing superresolution
    algorithm

22
Superresolution Framework
  • Apply superresolution algorithm post-processing
    to the 2-D MRI datasets that creates higher
    resolution in the slice-select dimension, thus
    creating a high-resolution, 3-D image of the
    object
  • First, a number of 2-D slice datasets are
    obtained, each shifted by a specified subpixel
    amount in the slice-select dimension relative to
    the other volume sets so as to create an
    isotropic volume resolution
  • Then, merge data and implement superresolution
    algorithm, yielding a high resolution version
  • Recursively implement algorithm until desired SNR
    is achieved

23
Superresolution Framework
Courtesy P. Kornprobst
24
Some Examples of Superresolution Algorithms
  • Recursive Least Squares (RLS)
  • Maximum Likelihood Restoration (ML)
  • Maximize conditional pdf given the ideal image
  • Maximum A Posteriori Estimator (MAP)
  • Maximize conditional pdf of the ideal image given
    the measurements
  • Irani-Peleg Iterative Back-Projection Algorithm
    (IBP)
  • See paper for more descriptions

25
IBP Framework
Is the MS difference between the actual
low-resolution images and the estimated
low-resolution images less than a desired
threshold?
Create the low resolution images
Hypothesize the high resolution image
End the Iterative Process
YES
NO
Update the best estimate of the
high-resolution image
n n 1
  • Irani-Peleg back-projection flow diagram

26
Image Sequence and MRI-Derived Superresolution
Results
  • Image Sequence (CCD and Video Camera) and
    MRI-based are under different circumstances,
    parameters, and assumptions, so the results
    cannot be compared directly
  • It will be shown in each cases associated
    reference frame that superresolution is beneficial

27
Video Imaging Analysis
  • Recursive Least Squares approach (Kim et al.)
  • Initial low resolution data 16 images of 40x40
    pixels, each subpixel uniformly shifted
  • Also, has additive white zero mean Gaussian noise
    of variance .001 (process also works for
    non-noisy case)

28
Video Imaging Analysis
Input Image is lenna 16-40x40 pixel images each
subpixel shifted Additive Gaussian White Noise
with variance 0.001
29
Video Imaging Analysis
Top Left Output of Initial High Resolution Image
(80x80 pixels) PSNR of 17.76 dB Right
Recursive Updates of High Resolution Images
(progressing top left to bottom right) PSNR of
13th update is 19.28 dB
30
MRI Imaging Analysis
  • Analyze Greenspans IBP method
  • Comb-phantom and actual human brain results
  • Comb-phantom
  • Surrounded in doped water (doped with Gd-DTPA)
  • Fast-spin echo
  • 16 slices of resolution 1mm x 1mm x 3mm
  • Slice-select (z) dimension parallel to teeth
  • 3 sets of slices, each shifted by 1mm in the z
    dimension (high resolution output voxel 1mm x
    1mm x 1mm)

31
Phantom Analysis
a) Original Low-Resolution Data b) Interpolation
through zero-padding c) Interleaving 3 sets
only d) Superresolution using Box-PSF e)
Superresolution using Gaussian-PSF
32
Human Brain Analysis
  • Actual Human Brain
  • 3 sets of 22 slice-select shifted low resolution
    images (1.5mm x 1.5mm x 4.5mm)
  • Each set shifted by 1.5mm
  • Acquired high resolution (1.5mm x 1.5mm x 1.5mm)
    image for comparison purposes

33
Human Brain Analysis
Top Left Low Resolution Version Top Right
Zero-padded interpolated version Bottom Left
Superresolution Image using Box-PSF Bottom Right
Superresolution Using Gaussian-PSF Bottom Actual
High Resolution Image (note image has been
expanded vertically for viewing purposes)
34
Summary
  • Goals
  • To analyze whether superresolution could be
    applied to MRI, and if so, with what kinds of
    results
  • Use normal video imaging as a baseline for
    comparison

35
Summary
  • Results
  • Principle differences
  • In normal imaging, superresolution can be applied
    to all dimensions
  • In MRI Imaging, the properties of the encoding
    scheme only lead to superresolution being
    beneficial in the slice-select dimension
  • MRI and CCD imaging do not require complex image
    registration, while video imaging does require a
    complex registration process projective
    transform

36
Summary
  • Additional MRI Superresolution Characteristics
  • Can be accomplished either with 3-D stacks of
    data or 2-D slices
  • Main necessity is subvoxel shifts in the
    slice-select dimension
  • Having a blurring filter (PSF) that closely
    resembles the MRI imaging system along with the
    MRI image characteristics in the slice-select
    dimension yields a better process

37
Benefits of MRI Superresolution
  • Can acquire 2-D slices at a fraction of the time
    it takes to acquire 3-D volumes, yet still
    achieve the high resolution images through
    post-processing
  • Reduces patient time, MRI ON time, and operator
    time
  • Dramatically reduces associated costs
  • Enables more people access to the machines over a
    given time period
  • Same techniques can be applied to PET, CT

38
Conclusion - Extension
  • Limit on in-plane resolution enhancement due to
    Fourier-encoding
  • If the signal is not Fourier-encoded, it may be
    possible to remove the limit and allow for
    resolution enhancement in-plane
  • How to accomplish this encoding?
  • One method could be to wavelet encode the
    temporal signals

39
Wavelet Encoding (xy plane)
  • Superresolution can be employed as long as there
    is sufficient subvoxel overlap, with wavelets as
    basis function for encoding
  • Only a few processes currently where non-Fourier
    encoding is of use
  • Diffusion-Weighted Imaging (DWI) high resolution
    images are difficult to acquire because of large
    phase variations due to slight patient motion
    during the gradient application process
  • Diffusion-Tensor Imaging (DTI) variation of DWI
    in which at least 7 different images acquired for
    every slice, with at least 6 different directions
    of diffusion weighting

40
Wavelet vs. Fourier Encoding
  • Wavelets less sensitive to motion
  • SNR and resolution of wavelet-encoded signal can
    be less than/equal to Fourier-encoded signal
    (based on choice of basis wavelet functions)
  • Wavelets offer more flexibility (choice of basis
    based on application)

41
Concluding Remarks
  • Non-Fourier encoding is usually applied to
    slice-select dimension due to the amount of
    resolution enhancement possible
  • One can theoretically increase the in-plane
    resolution (such as needed for very small subject
    or for process with great motion)
  • These aformentioned processes lend themselves for
    the non-Fourier methods, but the tradeoff may be
    too great

42
Thank You
  • Any questions?
  • Please come see me for references (if desired)
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