Calculating MRI RF coil sensitivities using interpolation into an enlarged field of view

Patent metadata

Field	Value
Publication number	US-10353023-B2
Application number	US-201415102288-A
Country	US
Kind code	B2
Filing date	Nov 27, 2014
Priority date	Dec 10, 2013
Publication date	Jul 16, 2019
Grant date	Jul 16, 2019

Abstract

A magnetic resonance imaging (MRI) system ( 100 ) has a radio frequency system ( 114, 116, 120, 124, 126 ) for acquiring magnetic resonance data ( 142, 144, 156 ). The radio frequency system includes a coil ( 124 ) with multiple antenna elements ( 126 ). The MRI system further includes a processor ( 133 ) for controlling the magnetic resonance imaging system. Execution of instructions ( 140, 170, 172, 174 ) cause the processor to: acquire ( 200 ) calibration magnetic resonance data ( 142 ) from a first field of view within the imaging zone using the multiple antenna elements, calculate ( 202, 300, 302, 304, 400 ) modified magnetic resonance data ( 144 ) by interpolating the calibration magnetic resonance data to a second field of view, calculate ( 204, 500, 502, 504, 602 ) a coil sensitivity kernel ( 146 ) by deconvolving the modified magnetic resonance data, and calculate ( 206, 604, 610 ) a coil sensitivity ( 148 ) by transforming each coil sensitivity kernel into image space. The second field of view encompasses and is larger than the first field of view.

First claim

The invention claimed is:

1. A magnetic resonance imaging system, comprising:
a radio frequency system for acquiring magnetic resonance data of a subject within an imaging zone, wherein the radio frequency system comprises a coil with multiple antenna elements operable for acquiring the magnetic resonance data;
a non-transitory computer readable memory for storing machine readable instructions;
a processor for controlling the magnetic resonance imaging system, wherein execution of the machine readable instructions cause the processor to:
acquire calibration magnetic resonance data from a first field of view within the imaging zone using each of the multiple antenna elements;
calculate modified magnetic resonance data by interpolating the calibration magnetic resonance data to a second field of view within the imaging zone, wherein the second field of view encompasses and is larger than the first field of view;
calculate a coil sensitivity kernel for each of the multiple antenna elements by deconvolving the modified magnetic resonance data for each of the multiple antenna elements; and
calculate a coil sensitivity for each of the multiple antenna elements by transforming each coil sensitivity kernel into image space.

2. The magnetic resonance imaging system of claim 1 , wherein the modified magnetic resonance data is calculated by:
reconstructing a first magnetic resonance image for each antenna element using the calibration magnetic resonance data;
calculating a modified magnetic resonance image for each antenna element, wherein each modified magnetic resonance image is defined by the second field of view and is calculated by pasting the first magnetic resonance image into a null valued image; and
calculating the modified magnetic resonance data by Fourier transforming the modified magnetic resonance image.

3. The magnetic resonance imaging system of claim 1 , wherein the modified magnetic resonance data is calculated by interpolating the calibration magnetic resonance data for each of the multiple antenna elements to a predefined set of points in Fourier space, wherein the predefined set of points in Fourier space represent the second field of view.

4. The magnetic resonance imaging system of claim 3 , wherein the modified magnetic resonance data for each of the antenna elements comprises a first set of points in Fourier space, and wherein the predefined set of points in Fourier space comprises the first set of points in Fourier space.

5. The magnetic resonance imaging system of claim 4 , wherein execution of the instructions further cause the processor to generate the predetermined set of points in Fourier space by translating a unit cell.

6. The magnetic resonance imaging system of claim 1 , wherein the radio frequency system further comprises a body coil; wherein execution of the instructions further causes the processor to:
acquire body coil magnetic resonance data from the first field of view using the body coil during acquisition of the calibration magnetic resonance data, and
calculate modified body coil magnetic resonance data by interpolating the body coil magnetic resonance data to the second field of view; and
wherein the coil sensitivity kernel for each of the multiple antenna elements is deconvolved with respect to the modified body coil magnetic resonance data.

7. The magnetic resonance imaging system of claim 1 , wherein execution of the instructions cause the processor to deconvolve the coil sensitivity kernel for each of the multiple antenna elements by initially setting a reference image to a predetermined value; wherein execution of the instructions cause the processor to further deconvolve the coil sensitivity kernel for each of the multiple antenna elements by iteratively repeating the following steps:
calculate an intermediate coil sensitivity kernel by deconvolving the modified magnetic resonance data for each of the multiple antenna elements with respect to a Fourier transform of the reference image,
calculate an intermediate coil sensitivity for each of the multiple antenna elements by transforming each intermediate coil sensitivity kernel into image space, and
recalculate the reference image using the intermediate coil sensitivities and the calibration magnetic resonance data; and
wherein the iterative steps are repeated a predetermined number of time or when the reference image has converged within a predetermined statistical measure.

8. The magnetic resonance imaging system of claim 7 , wherein the predetermined value of the reference image is a uniform value.

9. The magnetic resonance imaging system of claim 1 , wherein the memory further contains pulse sequence data descriptive of a parallel imaging magnetic resonance technique, wherein execution of the instructions further cause the processor to:
acquire imaging magnetic resonance data using the pulse sequence data to control the magnetic resonance imaging system from the first field of view; and
reconstruct a magnetic resonance image using the imaging magnetic resonance data and the corrected coil sensitivity for each of the multiple antenna elements.

10. The magnetic resonance imaging system of claim 1 , wherein execution of the instructions further cause the processor to recalculate the coil sensitivity for each of the multiple antenna elements by reducing the coil sensitivity to the first field of view.

11. A method of operating a magnetic resonance imaging system, wherein the magnetic resonance imaging system comprises a radio frequency for acquiring magnetic resonance data of a subject from an imaging zone, wherein the radio frequency system comprises a coil with multiple antenna elements operable for acquiring the magnetic resonance data, wherein the method comprises the steps of:
acquiring calibration magnetic resonance data from a first field of view within the imaging zone using each of the multiple antenna elements;
calculating modified magnetic resonance data by interpolating the calibration magnetic resonance data to a second field of view within the imaging zone, wherein the second field of view encompasses and is larger than the first field of view;
calculating a coil sensitivity kernel by deconvolving the modified magnetic resonance data for each of the multiple antenna elements;
calculating a coil sensitivity for each of the multiple antenna elements by transforming each coil sensitivity kernel into image space;
acquiring imaging magnetic resonance data from the first field of view using a parallel imaging technique;
reconstructing the acquired imaging magnetic resonance data into a magnetic resonance image using the calculated coil sensitivity for each of the multiple antenna elements; and
controlling a display device to display the reconstructed magnetic resonance image.

12. The method of claim 11 , wherein the modified magnetic resonance data is calculated by:
reconstructing a first calibration magnetic resonance image for each antenna element using the calibration magnetic resonance data;
calculating a modified calibration magnetic resonance image for each antenna element, wherein each modified calibration magnetic resonance image is defined by the second field of view and is calculated by pasting the first calibration magnetic resonance image into a null valued image; and
calculating the modified magnetic resonance data by Fourier transforming the modified calibration magnetic resonance image.

13. A non-transitory computer-readable medium carrying machine readable instructions for a processor for controlling a magnetic resonance imaging system, wherein the magnetic resonance imaging system includes a radio frequency syste

Assignees

• Koninklijke Philips Nv

Inventors

• Nielsen Tim

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

• G01R33/5608 Primary

  Data processing and visualization specially adapted for MR, e.g. for feature analysis and pattern recognition on the basis of measured MR data, segmentation of measured MR data, edge contour detection on the basis of measured MR data, for enhancing measured MR data in terms of signal-to-noise ratio by means of noise filtering or apodization, for enhancing measured MR data in terms of resolution by means for deblurring, windowing, zero filling, or generation of gray-scaled images, colour-coded images or images displaying vectors instead of pixels (image data processing or generation, in general G06T) · CPC title

• G01R33/246 Primary

  Spatial mapping of the RF magnetic field B1 · CPC title