MR imaging with spiral acquisition

Patent metadata

Field	Value
Publication number	US-11959986-B2
Application number	US-201916979940-A
Country	US
Kind code	B2
Filing date	Mar 5, 2019
Priority date	Mar 13, 2018
Publication date	Apr 16, 2024
Grant date	Apr 16, 2024

Abstract

The invention relates to a method of MR imaging of an object (10) positioned in an examination volume of a MR device (1). It is an object of the invention to enable efficient spiral MR imaging even in situations of strong Bo inhomogeneity. The method of the invention comprises: subjecting the object (10) to an imaging sequence comprising at least one RF excitation pulse and sinusoidally modulated magnetic field gradients, acquiring MR signals along two or more spiral k-space trajectories (31, 32, 33) as determined by the sinusoidal modulation of the magnetic field gradients, wherein the origins of the spiral k-space trajectories are offset from each other, and reconstructing an MR image from the acquired MR signals. Moreover, the invention relates to a MR device (1) and to a computer program for a MR device (1).

First claim

The invention claimed is:

1. A method of magnetic resonance (MR) imaging of an object positioned in an examination volume of an MR device, the method comprising:
subjecting the object to an imaging sequence comprising at least one RF excitation pulse and sinusoidally modulated magnetic field gradients,
selecting two or more spiral k-space trajectories, wherein the origins of the spiral k-space trajectories are offset from each other in a plane of the spiral k-space trajectories, wherein the offset spiral k-space trajectories are overlapping in a region around k-space origin, wherein the origins of the spiral k-space trajectories are at least one of (i) offset from k-space origin, (ii) equally spaced from k-space origin, and (iii) symmetrically arranged around k-space origin, wherein each spiral k-space trajectory lies in a k x ,k y plane and the origins of the spiral k-space trajectories are offset from each other along a direction parallel with the k x ,k y plane;
acquiring MR signals along the two or more spiral k-space trajectories;
reconstructing an MR image from the acquired MR signals; and
displaying the MR image.

2. The method of claim 1 , wherein the origins of the spiral k-space trajectories are offset from k-space origin.

3. The method of claim 1 , wherein the origins of the spiral k-space trajectories are equally spaced from k-space origin.

4. The method of claim 3 , wherein the origins of the spiral k-space trajectories are symmetrically arranged around k-space origin.

5. The method of claim 1 , wherein a B 0 map is derived from the MR signals, acquired from the region around k-space origin.

6. The method of claim 5 , wherein the MR image is reconstructed with correction of B 0 inhomogeneity based on the derived B 0 map.

7. The method of claim 1 , wherein the object is subjected to a preparation sequence prior to the imaging sequence, wherein a B 0 map is derived from MR signals acquired during the preparation sequence.

8. The method of claim 7 , wherein at least one of the number or the arrangement of the spiral k-space trajectories in k-space is chosen automatically depending on the B 0 map.

9. The method of claim 1 , wherein the MR signals are acquired according to a stack-of-spirals scheme from a number of parallel k-space slices arranged at adjacent positions along a direction perpendicular to the k-space slices.

10. The method of claim 1 , wherein the MR signals are acquired at two or more different echo times, wherein signal contributions from water protons and fat protons are separated in the step of reconstructing the MR image.

11. The method of claim 1 , wherein k-space is sampled in three dimensions by the two or more spiral k-space trajectories.

12. A magnetic resonance (MR) device comprising:
at least one main magnet coil for generating a uniform, static magnetic field within an examination volume;
gradient coils for generating switched magnetic field gradients in different spatial directions within the examination volume;
at least one RF coil for generating RF pulses within the examination volume and/or for receiving MR signals from an object positioned in the examination volume;
a control unit for controlling a temporal succession of the RF pulses generated by the at least one RF coil and the switched magnetic field gradients generated by the gradient coils;
a video monitor; and
a reconstruction unit for reconstructing a MR image from the received MR signals, wherein the MR device is arranged to perform the following steps:
subjecting the object to an imaging sequence comprising at least one RF excitation pulse and sinusoidally modulated magnetic field gradients,
selecting two or more spiral k-space trajectories, wherein each spiral k-space trajectory lies in a k x -k y plane and the origins of the spiral k-space trajectories are offset from each other in the k x and/or k y directions, wherein the offset spiral k-space trajectories are overlapping in a region around k-space origin;
acquiring MR signals along the two or more spiral k-space trajectories;
reconstructing an MR image from the acquired MR signals; and
displaying the MR image on the video monitor.

13. A computer program stored on a non-transitory computer readable medium, to be run on a magnetic resonance (MR) device, which computer program comprises instructions for:
generating an imaging sequence comprising at least one RF excitation pulse and sinusoidally modulated magnetic field gradients;
selecting MR signals along two or more spiral k-space trajectories, wherein each spiral k-space trajectory lies in a k x -k y plane and the origins of the spiral k-space trajectories are offset from each other along a direction parallel with the k x -k y plane, wherein the offset spiral k-space trajectories are overlapping in a region around k-space origin;
acquiring MR signals along the two or more spiral k-space trajectories;
reconstructing an MR image from the acquired MR signals; and
displaying the MR image.

14. The method of claim 1 , wherein the origins of the spiral k-space trajectories are offset from each other in the k x and/or k y directions.

Assignees

• Koninklijke Philips Nv

Inventors

• Fuderer Miha
• Hey Silke

Classifications

• G01R33/4826 Primary

  in three dimensions · CPC title

• G01R33/243

  Spatial mapping of the polarizing magnetic field · CPC title

• G01R33/4828

  Resolving the MR signals of different chemical species, e.g. water-fat imaging · CPC title

• G01R33/56563

  caused by a distortion of the main magnetic field B0, e.g. temporal variation of the magnitude or spatial inhomogeneity of B0 (G01R33/56509, G01R33/56518, G01R33/56536 take precedence) · CPC title

• G01R33/4824 Primary

  using a non-Cartesian trajectory · CPC title