Patient-adaptive B0 homogenization of MR systems using different types of shim coils

Patent metadata

Field	Value
Publication number	US-9851423-B2
Application number	US-201414464073-A
Country	US
Kind code	B2
Filing date	Aug 20, 2014
Priority date	Aug 21, 2013
Publication date	Dec 26, 2017
Grant date	Dec 26, 2017

Abstract

The embodiments relate to methods and to magnetic resonance tomography systems having a shim system, where the shim system includes at least one global shim coil in an area surrounding the bore of the magnetic resonance tomography system, and where the shim system includes a local shim coil in a local coil of the magnetic resonance tomography system with a shim controller, where the shim controller embodied to define shim currents for the global shim coil and for the local shim coil.

First claim

The invention claimed is:

1. A magnetic resonance tomography (MRT) system comprising:
a shim system comprising:
at least one global shim coil in an area surrounding a bore of the magnetic resonance tomography system;
at least one local shim coil in a local coil of the magnetic resonance tomography system; and

a shim controller configured to determine global shim currents for the global shim coil and local shim currents for the local shim coil,
wherein the shim controller is configured to determine the global shim currents and the local shim currents using a three-dimensional linear combination of shim fields created with the at least one global shim coil and the at least one local shim coil with an optimization method for searching for a minimization of the basic field inhomogeneity caused by the shim currents of the at least one global shim coil and the at least one local shim coil.

2. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim system comprises a plurality of global shim coils in the area surrounding the bore, a plurality of local shim coils in the local coil, or a plurality of global shim coils in an area surrounding the bore and a plurality of local shim coils in the local coil.

3. The magnetic resonance tomography system in claim 1 , further comprising:
a global shim coil memory comprising global shim coil data relating to shim characteristics of the at least one global shim coil, field distribution data relating to a spatial field distribution of a shim field, or a combination thereof;
a local shim coil memory comprising local shim coil data relating to shim characteristics of the at least one local shim coil, field distribution data relating to a spatial field distribution of a shim field created with the at least one local shim coil, or a combination thereof; or
a combination thereof,
wherein the shim controller is configured to determine the global shim currents and the local shim currents using the global shim coil data and the local shim coil data.

4. The magnetic resonance tomography system as claimed in claim 1 , wherein the at least one global shim coil, the at least one local shim coil, or both the at least one global shim coil and the at least one local shim coil are configured to provide field distribution data relating to a spatial field distribution of a shim field,
wherein the field distribution data is stored outside the local coil.

5. The magnetic resonance tomography system as claimed in claim 1 , wherein the at least one local shim coil is configured to provide field distribution data relating to a spatial field distribution of a shim field,
wherein the field distribution data is stored in a memory in the local coil.

6. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim controller is configured to determine the global shim currents and the local shim currents using: (1) the local shim coil position data representing a position of the local shim coil; (2) data representing a type of the local shim coil; or (3) both the local shim coil position data representing the position of the local shim coil and the data representing the type of the local shim coil.

7. The magnetic resonance tomography system as claimed in claim 1 , wherein the at least one global shim coil, the at least one local shim coil, or both the at least one global shim coil and the at least one local shim coil are configured to provide field distribution data relating to a spatial field distribution of a shim field,
wherein the spatial field distribution is provided as a three-dimensional field map, as a pixel map, or as coefficients of functions.

8. The magnetic resonance tomography system as claimed in claim 1 , wherein global shim coil data, local shim coil data, or global shim coil and local shim coil data specify a sensitivity of at least one shim coil by how much magnetic field is able to be created per ampere of shim current in the at least one shim coil.

9. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim controller is configured to determine the global shim currents and the local shim currents: (1) using a stored B 0 field distribution of a basic field previously created by a basic field magnet of the MRT alone; (2) without field generation by shim coils determined in an adjustment measurement; or (3) using the stored B 0 field distribution of the basic field and without field generation by shim coils determined in the adjustment measurement.

10. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim controller is configured to determine the global shim currents and the local shim currents using stored shim field strengths created for the global shim coil and the local shim coil measured per unit of shim current.

11. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim controller is configured to determine the global shim currents and the local shim currents using a field distribution of a shim field created with the local shim coil through the shim current and position data representing a position of the local shim coil.

12. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim controller is configured to determine the global shim currents and the local shim currents using field distribution data representing a field distribution of a shim field created with the local shim coil by the shim current,
wherein the shim field for a shim coil comprises three files in each case,
wherein each file represents field distribution data relating to a field distribution in the direction of one of three base vectors orthogonal to one another of a shim space and as a linear combination together represents the field distribution of a shim field able to be created with the shim coil.

13. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim controller is configured to determine the global shim currents and the local shim currents using stored data relating to a field error created by a patient to be examined, representing a change of the basic field.

14. The magnetic resonance tomography system as claimed in claim 13 , wherein the stored data comprises three files,
wherein each file represents field distribution data relating to a change of the field distribution in the direction of one of three base vectors, orthogonal to one another of a possible shim space and as a linear combination together represents the change of the field distribution of the basic field.

15. The magnetic resonance tomography system as claimed in claim 1 , wherein the global shim currents are defined for the global shim coil in order to reduce large-area inhomogeneities, and
wherein a new field map is determined that takes account of shim fields created by the global shim currents in the global shim coil and a basic field inhomogeneity caused by a patient to be examined and the basic field, and the local shim currents are defined for the local shim coil.

16. The magnetic resonance tomography system as claimed in claim 15 , wherein the new field map takes account of the shim fields only in the area of the patient to be examined.

17. The magnetic resonance tomography system as claimed in claim 1 , wherein the shim controller is configured to determine the global shim currents from a B 0 field distribution, determined in an adjustment measurement, of a basic field created by basic field magnets of the MRT alone, without field generation by shim coils, or by the basic field magnets of the MRT and without

Assignees

• Biber Stephan
• Ladebeck Ralf
• Siemens Ag

Inventors

• Biber Stephan
• Ladebeck Ralf

Classifications

• G01R33/3875 Primary

  using correction coil assemblies, e.g. active shimming · CPC title

• A61B5/0522

  Magnetic induction tomography · CPC title

• A61B5/055 Primary

  involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging · CPC title

• G01R33/445

  MR involving a non-standard magnetic field B0, e.g. of low magnitude as in the earth's magnetic field or in nanoTesla spectroscopy, comprising a polarizing magnetic field for pre-polarisation, B0 with a temporal variation of its magnitude or direction such as field cycling of B0 or rotation of the direction of B0, or spatially inhomogeneous B0 like in fringe-field MR or in stray-field imaging · CPC title

• A61B5/704

  Tables · CPC title