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Parallel Imaging Meeting 2005

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Higher speed in MRI is desirable due to cost, time limitations, and the motion artifacts. It is possible ... Median filtering & low-pass homomorphic filtering ... – PowerPoint PPT presentation

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Title: Parallel Imaging Meeting 2005


1
Parallel Imaging Meeting 2005
  • Esin Ozturk
  • UCSF/UCB Joing Graduate Group in Bioengineering

2
Parallel MRI
  • Higher speed in MRI is desirable due to cost,
    time limitations, and the motion artifacts.
  • It is possible to reduce the scan time by faster
    phase encoding.
  • Gradient switching rate has a limit.
  • Neuromuscular stimulation might be a problem.
  • Acquiring multiple MR data points simultaneously
    can result in the possibility of reducing the
    acquired data, and retrieving it in the
    reconstruction phase using parallel imaging
    techniques.

3
Main Idea
  • Multiple receiver coils to acquire the MR signal
    simultaneously.
  • Reduced phase encode steps acquired from each
    coil to reduce the data acquisition time by
    keeping kmax same and increasing ?k by a factor
    of 2.
  • Signal induced in an RF coil varies by the
    distance between the signal source and the coil.
    ? Coil Sensitivity
  • Special image reconstruction techniques employing
    coil sensitivities methods like SENSE, GRAPPA
    etc.

4
Overview of Steps
DATA ACQ/PREPARATION
Simulation - Image - Spectra
DATA RECONSTRUCTION
SENSE GRAPPA AUTO-SMASH VD-AUTO-SMASH
5
Sensitivity Encoding (SENSE)
6
Principles of SENSE
  • A set of receiver coils are used to acquire
    undersampled k-space data.
  • These data are inverse Fourier transformed
    directly which results in half FOV images/spectra
    in the reduction direction for R2.
  • Each pixel in an aliased image is a superposition
    of multiple pixels from a full unaliased image.
  • Knowing the coil sensitivities of all the pixels
    contributing to the pixel, and the composite end
    value, it is possible to solve a linear equation
    for each pixel.

7
1. Combining multi-channel data R1
x

Coil sensitivities at voxel v
Data of each coil element at voxel v
8
2. Combining with SENSE for R2
x

Coil sensitivities at voxel v
Data of each coil element at voxel v
9
Simulations Original Image
Modified Shepp-Logan phantom (256256)
10
Simulations Coil Sensitivity Maps
  • Coil sensitivities are simulated as Gaussian
    functions with FWHM5cm
  • and max height 1 at a FOV 15cm
  • Sensitivity

11
Intermediate SENSE Images
  • Phase encoding step size 2
  • ?k ? ?k 2
  • ? FOV1/dk ? FOV / 2
  • Direct 2D IFT results in reduced FOV aliased
    images.

Simulated intermediate images from 3 seperate
coils
12
Reconstructed Image
13
Empirical Coil Sensitivity Maps
  • For the calibration image of a given coil
    element
  • Divide by the masked combined image
  • Median filtering low-pass homomorphic
    filtering
  • Dilate by a 3x3 kernel to extend the image for
    edge preservation.
  • Division by the body coil images or theorotical
    maps ?

14
SENSE Spectroscopy
  • Spectroscopic data can be viewed as a 4
    dimensional data, where three of the dimensions
    are spatial, and the fourth is the spectral
    dimension.
  • After 1D FFT of the spectral, and 3D IFFT of the
    spatial domains, we can apply SENSE
    reconstruction for each voxel at each spectral
    point on a slice by slice basis.

15
Aliasing of spectra
  • SIMULATION
  • 3232 Full FOV
  • 1616 1/4th FOV
  • Fourier reconstruction applied
  • Peaks of A, B, C, D
  • A is the superimposed pixel.

Figure 1 in Dydak et al.s paper
16
SENSE reconstruction for spectra
  • Phantom filled with Cre of 10 mmol/l, Glass
    spheres NAA 10 mmol/l, Cre 20 mmol/l, Lac 10
    mmol/l
  • Creatine map with full FOV
  • Aliased creatine map acquired with half FOV,
    voxel A is a weighted sum of the 4 marked voxels.
  • SENSE reconstructed

Figure 4 of Dydak et al.s paper
17
Spectral Simulation
phase encode direction
18
Lipid Unaliasing using SENSE
  • For a given voxel within the FOV
  • Possible aliasing voxels (FOV away from the
    voxel) were determined.
  • Voxels within the head region were selected.
  • Original spectral array (FOVxFOV) was treated as
    a half FOV representation of an extended spectral
    array (2FOVx2FOV).
  • Using
  • 8 sets of coil sensitivities, and
  • 8 spectral values of the given voxel from the
    different channels
  • the spectra in the original and the aliasing
    voxels were resolved.

19
Example Grade 4 Glioma Patient
20
Problems of SENSE
  • SENSE requires the inversion of matrices that
    might result in computational errors.
  • SENSE is computationally expensive because
    unfolding is performed for each pixel.
  • Noise can cause reconstruction errors.
  • Reduction factor (R) can not exceed the number of
    coils.
  • SNR is reduced by a factor of at least ? R
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