System and method for externally calibrated parallel imaging in the presence of an inhomogeneous magnetic field

Patent metadata

Field	Value
Publication number	US-2016154080-A1
Application number	US-201414558374-A
Country	US
Kind code	A1
Filing date	Dec 2, 2014
Priority date	Dec 2, 2014
Publication date	Jun 2, 2016
Grant date	—

Abstract

A system and method for accelerated magnetic resonance imaging (MRI) includes controlling an RF system of an MRI system to acquire coil calibration data from a subject including a material causing inhomogeneities in a static magnetic field of the MRI system when arranged in the bore of the MRI system. After acquiring the coil calibration data, the RF system is controlled to acquire imaging data from the subject at multiple different resonance frequency offsets. The spectral bin images relate specific resonance frequencies to distinct spatial locations in the static magnetic field of the MRI system. An image of the subject is reconstructed from the imaging data using coil calibration data and the spectral bin data to provide spatial encoding of the image.

First claim

1 . A magnetic resonance imaging (MRI) system comprising:
a magnet system configured to generate a static magnetic field about at least a bore of the MRI system; a plurality of gradient coils configured to apply a gradient field to the static magnetic field; a radio frequency (RF) system including an array of coils configured to apply an excitation field and acquire MR image data therefrom; a computer system configured to:
control the RF system to acquire coil calibration data from a subject including a material causing inhomogeneities in the static magnetic field when arranged in the bore of the MRI system;
after acquiring the coil calibration data, control the RF system to acquire imaging data with from the subject;
analyze the imaging data to generate spectral bin data with respect to a plurality of spectral bins, wherein the spectral bin data relates specific resonance frequencies to distinct spatial locations in the static magnetic field of the MRI system; and
reconstruct an image of the subject from the imaging data using the coil calibration data and the spectral bin data to provide spatial encoding of the image for each spectral bin.

2 . The system of claim 1 wherein, to acquire the imaging data, the computer system is configured to undersample a center of k-space and a periphery of k-space.

3 . The system of claim 1 wherein, to acquire the coil calibration data, the computer system is configured to fully sample a center of k-space.

4 . The system of claim 1 wherein, to generate the spectral bin data, the computer system is configured to produce a plurality of images at different resonance frequencies using the calibration data and the spectral bin data, each of the plurality of images depicting spatial locations within an imaging field-of-view of the MRI system that are associated with a particular spectral response.

5 . The system of claim 4 wherein the particular spectral response is a range of resonance frequencies that are off-resonance because of the inhomogeneities in the static magnetic field of the MRI system.

6 . The system of claim 1 wherein, to acquire the imaging data, the computer system is configured to:
i) apply a radio frequency (RF) excitation pulse having a center frequency and a spectral bandwidth;
ii) acquire an imaging data set following the application of the RF excitation pulse; and
iii) repeating steps a)i) and a)ii) a plurality of times to acquire the imaging data while changing at least one of the center frequency and the spectral bandwidth of the RF excitation pulse during each repetition of step i).

7 . The system of claim 6 wherein, to generate the spectral bin data, the computer system is configured to reconstruct a spectral bin image from each imaging data set and wherein each spectral bin image depicts spatial locations within an imaging field-of-view of the MRI system that are associated with resonance frequencies in a spectral band defined by the center frequency and spectral bandwidth of the RF excitation pulse associated with the k-space data set from which the spectral bin image was reconstructed.

8 . The system of claim 6 wherein for each repetition of ii), the computer system is further caused to sample k-space with a different sampling pattern.

9 . The system of claim 8 wherein the computer system is further caused to select each different sampling pattern to adjust at least one of a center frequency and spectral bandwidth of the RF excitation pulse associated with the imaging data set being acquired.

10 . The system of claim 1 wherein the computer system is further caused to control the gradient system to apply a magnetic field gradient to amplify the inhomogeneities in the magnetic field.

11 . A method for acquiring imaging data from multiple different resonance frequency offsets with a magnetic resonance imaging (MRI) system, the method including steps comprising:
a) acquiring coil calibration data using a coil array positioned for imaging with respect to a subject having a material causing inhomogeneities in a static magnetic field of the MRI system; b) separately from acquiring the coil calibration data, acquiring imaging data from the subject across a plurality of different resonance frequency offsets corresponding to respective spectral bins; c) deriving spectral bin images from the imaging data, wherein the spectral bin images relate specific resonance frequencies to distinct spatial locations in the static magnetic field of the MRI system; and d) reconstructing spectral bin images of the subject from the imaging data using coil calibration data and the spectral bin images to provide spatial encoding of the spectral bin images.

12 . The method of claim 11 wherein step b) includes:
i) producing a multiband radio frequency (RF) pulse or a single-band pulse that excites spins associated with each of the plurality of different resonance frequency offsets;
ii) establishing a first phase-encoding gradient along a first direction;
iii) establishing a second phase-encoding gradient along a second direction that is orthogonal to the first direction;
iv) establishing a third phase-encoding gradient along a third direction that is orthogonal to the first direction and the second direction; and
v) acquiring data at a point in k-space that is defined by the first, second, and third phase-encoding gradients by sampling a magnetic resonance signal during a period of time in which no magnetic field gradients are established by the MRI system.

13 . The method of claim 12 wherein the plurality of different resonance frequency offsets includes an on-resonance RF offset and at least one off-resonance RF offset.

14 . The method of claim 12 further comprising producing a multiband or single band refocusing RF pulse that refocuses magnetization attributable to the excited spins associated with each of the plurality of resonance frequency offsets so as to form the magnetic resonance signal as a spin-echo at an echo time.

15 . The method of claim 12 wherein the magnetic resonance signal includes a free-induction decay signal, a spin-echo signal, or a stimulated echo signal.

16 . The method of claim 12 , further comprising repeating steps i)-v) a plurality of times while each repetition alters at least one of the first, second, and third phase-encoding gradients such that data are acquired from a different point in k-space during each repetition, the different points in k-space defining a k-space sampling pattern.

17 . The method of claim 16 wherein the k-space sampling pattern includes undersampling k-space all regions of k-space using at least one of a Cartesian grid, radial lines, spiral trajectories, or randomly distributed in three-dimensional k-space.

18 . The method of claim 17 wherein the k-space sampling pattern includes a variable density of sampling points such that different portions of k-space are undersampled with different sampling densities.

19 . The method of claim 17 wherein at least a center of k-space is fully sampled to acquire the coil calibration data.

20 . The method claim 11 wherein step a) includes generating a coil calibration map that spans the plurality of different resonance frequency offsets.

Assignees

• Wisconsin Alumni Res Found

Inventors

• Wiens Curtis N
• Artz Bartlett S

Classifications

• G01R33/5611

  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

• G01R33/483

  with selection of signals or spectra from particular regions of the volume, e.g. in vivo spectroscopy · CPC title

• G01R33/246

  Spatial mapping of the RF magnetic field B1 · CPC title

• G01R33/56536 Primary

  due to magnetic susceptibility variations · CPC title

• G01R33/5659

  caused by a distortion of the RF magnetic field, e.g. spatial inhomogeneities of the RF magnetic field (G01R33/56509, G01R33/56518, G01R33/56536 take precedence) · CPC title