System and method for z-shim compensated echo-planar magnetic resonance imaging
US-2016209487-A1 · Jul 21, 2016 · US
US9778336B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9778336-B2 |
| Application number | US-201414180026-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 13, 2014 |
| Priority date | Feb 13, 2013 |
| Publication date | Oct 3, 2017 |
| Grant date | Oct 3, 2017 |
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A system and method for medical imaging using a magnetic resonance imaging system includes performing a segmented echo planar imaging (EPI) pulse sequence. The pulse sequence includes performing multiple radio frequency (RF) excitation pulses designed to excite multiple imaging slices across the subject simultaneously. A gradient encoding scheme applied along the slice-encoding direction is implemented to impart controlled phase shifts to the different imaging slices. Additionally, the multiple RF excitation pulses can be designed to further control an overlap of imaging data acquired from adjacent slices of the multiple imaging slices based on a selected offset. The acquired imaging data is reconstructed using a parallel imaging reconstruction method that separates overlapped slices in the imaging data to provide a series of images with respective images for each of the multiple imaging slices across the subject.
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The invention claimed is: 1. A method for producing a series of images of a subject associated with a plurality of different slice locations using a magnetic resonance imaging (MRI) system, the steps of the method comprising: a) directing the MRI system to perform a pulse sequence that includes: generating a radio frequency (RF) excitation field that simultaneously excites spins in a plurality of different slice locations; establishing a first magnetic field gradient sequence along a first direction to form magnetic resonance signals from the excited spins; establishing a second magnetic field gradient sequence during the first magnetic field gradient sequence and along a second direction orthogonal to the first direction, wherein the first and second magnetic field gradient sequences define a k-space trajectory that traverses a segment of k-space; establishing a third magnetic field gradient sequence during the first magnetic field gradient sequence and along a third direction orthogonal to the first and second directions, wherein the third magnetic field gradient sequence imparts a phase shift to the formed magnetic resonance signals along one of the first and second directions; b) acquiring first k-space data from the segment of k-space, the first k-space data being indicative of the plurality of different slice locations; c) repeating a) and b) to acquire second k-space data from a different segment of k-space, wherein during the repetition of step a) at least one of the first and second magnetic field gradient sequences is modified to define a different k-space trajectory that traverses a different segment of k-space and wherein additional data is acquired from a given slice location by sampling a different segment of k-space; and d) reconstructing a series of images from the first and second k-space data, the series of images including images associated with the plurality of different slice locations. 2. The method as recited in claim 1 , wherein the third magnetic field gradient sequence comprises a plurality of magnetic field gradient blips. 3. The method as recited in claim 2 , wherein at least some of the plurality of magnetic field gradient blips have a different polarity than others of the plurality of magnetic field gradient blips. 4. The method as recited in claim 2 , wherein at least some of the plurality of magnetic field gradient blips have a different magnitude than others of the plurality of magnetic field gradient blips. 5. The method as recited in claim 2 , wherein at least some of the plurality of magnetic field gradient blips have a different magnitudes and polarities than others of the plurality of magnetic field gradient blips. 6. The method as recited in claim 1 , wherein step c) includes modifying the third magnetic field gradient sequence during the repetition of step a) to impart a different phase shift to the formed magnetic resonance signals. 7. The method as recited in claim 1 , wherein the first magnetic field gradient sequence comprises an alternating magnetic field gradient. 8. The method as recited in claim 1 , wherein the second magnetic field gradient sequence comprises a plurality of magnetic field gradient blips. 9. The method as recited in claim 1 , wherein the second magnetic field gradient sequence comprises a constant magnetic field gradient. 10. The method as recited in claim 1 , wherein the second magnetic field gradient sequence comprises an alternating magnetic field gradient. 11. The method as recited in claim 1 , wherein the k-space trajectory is a Cartesian trajectory. 12. The method as recited in claim 1 , wherein the k-space trajectory is a spiral trajectory. 13. The method as recited in claim 1 , wherein the RF excitation field is generated in step a) using a multiband RF pulse that includes a plurality of different sub-pulses, each of the plurality of different sub-pulses being associated with one of the plurality of different slice locations. 14. The method as recited in claim 13 , wherein step c) includes modifying the multiband RF pulse used in the repetition of step a) to generate a different RF excitation field that excites the spins in the plurality of different slice locations while imparting an additional phase shift to the formed magnetic resonance signals. 15. The method as recited in claim 14 , wherein modifying the multiband RF pulse comprises modifying a phase of at least one of the plurality of different sub-pulses. 16. The method as recited in claim 15 , wherein modifying the phase of at least one of the plurality of different sub-pulses comprises adding a phase shift to the at least one of the plurality of different sub-pulses. 17. The method as recited in claim 16 , wherein the phase shift added to the at least one of the plurality of different sub-pulses is a 180 degree phase shift. 18. The method as recited in claim 1 , wherein step d) includes reconstructing the series of images using a reconstruction algorithm that accounts for the controlled aliasing imparted to the first and second k-space data. 19. The method as recited in claim 18 , wherein the reconstruction algorithm includes a slice-GRAPPA reconstruction algorithm.
using gradient refocusing, e.g. EPI · CPC title
of multiple slices · CPC title
Parallel magnetic resonance imaging, e.g. sensitivity encoding [SENSE], simultaneous acquisition of spatial harmonics [SMASH], unaliasing by Fourier encoding of the overlaps using the temporal dimension [UNFOLD], k-t-broad-use linear acquisition speed-up technique [k-t-BLAST], k-t-SENSE (structural details of arrays of sub-coils G01R33/3415) · CPC title
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