Method and apparatus for producing homogeneous magnetic fields

• US 8,712,706 B2
• Filed: 12/01/2010
• Issued: 04/29/2014
• Est. Priority Date: 12/02/2009
• Status: Active Grant

• Current Assignee: Nanalysis Corp. (Nanalysis Scientific Corp.)
• Original Assignee: Nanalysis Corp. (Nanalysis Scientific Corp.)
• Inventors: Leskowitz, Garett M., McFeetors, Gregory, Pernecker, Sebastien
• Primary Examiner(s): Kundu, Sujoy
• Assistant Examiner(s): FORTICH, ALVARO E
• Application Number:
  US12/957,987
• Publication Number:
  US 20110137589A1
• Time in Patent Office: 1,245 Days
• Field of Search: 702115-117, 702/106
• US Class Current: 702/57
• CPC Class Codes: G01R 33/3875 using correction coil assemblies, e.g. active shimming

Abstract

A method for shimming a magnetic field is disclosed. The method uses a single shim current to contribute to suppression of more than one geometrical component of an inhomogeneity in the magnetic field without changing the geometry of the shim path. Apparatuses to implement the method are also disclosed. In embodiments the apparatuses comprise substantially commonly oriented shim paths.

Claims

1. A method for shimming a magnetic field in which there is an inhomogeneity having more than one functional component, the magnetic field being produced by a magnet assembly having two opposed and mutually distanced assembly ends and an assembly axis, the method comprising:

providing a plurality of commonly oriented shim paths, said shim paths disposed on a common surface having two opposed and mutually distanced ends, each of said surface ends having at least one associated electrical connector;

applying a plurality of coordinately modulated single electronic shim currents along corresponding ones of the plurality of shim paths, each of said electronic shim currents entering said electrical connector at one said surface end, flowing from said electrical connector at said one said surface end to said electrical connector at the other said surface end, and exiting said electrical connector at the other said surface end; and

;

suppressing the more than one functional component of the inhomogeneity in the magnetic field using the plurality of electronic shim currents;

wherein each of said surface ends is proximate a corresponding one of said assembly ends so that at least a portion of said shim currents flows from one said assembly end towards the other said assembly end.

2. The method according to claim 1, wherein each individual one of the plurality of electronic shim currents flows in a respective one of the plurality of shim paths, and wherein the individual ones of the currents are determined by:

estimating a magnetic field produced by application of a known current to each of the plurality of shim paths;

computing a scalar product of functions representative of the functional components of the estimated magnetic field to obtain functional component values;

arranging the functional component values into a matrix;

determining a pseudoinverse of the matrix to obtain pseudoinverse matrix values; and

choosing the individual ones of the currents according to the pseudoinverse matrix values.

3. The method according to claim 1, wherein said applying comprises coordinately adjusting the magnitudes of said electronic shim currents.

10. The method according to claim 1, wherein the plurality of said shim paths are mutually connected at one of said surface ends and said mutually connected path ends are held at a grounding electric potential controlled by external electronic means.

11. The method according to claim 1, wherein said magnet assembly has an assembly axis and a sample is inserted into said magnetic field along said assembly axis.

16. The method according to claim 2, wherein said applying comprises coordinately adjusting the magnitudes of said electronic shim currents.

17. The method according to claim 1, wherein said magnet assembly at least partly defines a sample volume.

4. A detector for detecting magnetic resonance in a sample exposed to a main magnetic field, the detector comprising:

a substantially flat shim panel having two opposed and mutually distanced panel ends and a panel axis, each of said two ends having one or more associated electrical connectors, the shim panel comprising a plurality of shim paths having a substantially common orientation extending between said two panel ends, the shim paths for applying electronic shim currents thereon, each of said currents entering an electrical connector at one said panel end, flowing from said electrical connector at said one said panel end to an electrical connector at the other said panel end, and exiting said electrical connector at the other said panel end.

5. The detector according to claim 4, further comprising a longitudinal space having an axis, the longitudinal space for insertion of a sample probe containing the sample along the axis and wherein the orientation is substantially parallel to the axis.

6. The detector according to claim 5, further comprising at least two said flat shim panels, each mounted on separate ones of two pole pieces, the said pole pieces extending within the longitudinal space.

7. The detector according to claim 4, wherein at least a subset of the plurality of shim paths are disposed on substantially parallel surfaces of the shim panel.

8. The detector according to claim 4, further comprising a printed circuit board on which is comprised the flat shim panel.

18. The detector according to claim 4, wherein said magnetic field is at least partly produced by a magnet assembly having two opposed and mutually distanced assembly ends and an assembly axis, and wherein each of said two panel ends is proximate one of said assembly ends.

22. The detector according to claim 4, wherein said magnet assembly is adapted to receive a sample inserted into said magnetic field along said assembly axis, and wherein said panel axis coincides with or is substantially parallel to said assembly axis.

9. A shim panel comprising a printed circuit board having first and second substantially distanced and mutually opposed panel ends and a substantially flat portion comprising a plurality of electrical current conducting shim paths extending between and terminating at said panel ends, wherein individual ones of the shim paths have a substantially common orientation, wherein said electrical current enters each of said shim paths at one said panel end and is conducted along each of said shim paths and exits each of said shim paths at the other of said panel ends.

19. The shim panel according to claim 9, wherein said panel is adapted so that said panel is positionable in a channel within a cooperating magnet array so that said electrical current carrying shim paths extend through the channel.

20. The shim panel according to claim 19, wherein each of said panel ends comprises an electrical connector accessible from a corresponding end of the channel.

12. A method for constructing a set of desired magnetic field configurations within a magnetic resonance apparatus comprising a plurality of shim paths, the method comprising the steps of:

(a) providing a shim panel having first and second substantially distanced panel ends and a substantially flat portion, said shim panel adapted to comprise at least a subset of said shim paths such that individual ones of said subset of said shim paths each substantially extend between said panel ends, wherein individual ones of the shim paths have a substantially common overall orientation, and wherein said subset of said shim paths are configured for applying electronic shim currents thereon, each of said currents entering a shim path at one said panel end, flowing along said shim path from said one said panel end and exiting said shim path at the other said panel end;

(b) estimating a representation of the magnetic field as a function of spatial coordinate variables produced by a known electronic shim current in a first one of said shim paths by integrating the Biot-Savart equation;

(c) computing a scalar product of (i) a desired magnetic field configuration, and (ii) a magnetic field function estimated according to step (b);

(d) repeating step (b) and step (c) for a plurality of pairs of said desired magnetic field configurations and estimated shimming field functions produced by known electronic shim currents;

(e) arranging the scalar product values of step (d) into a matrix;

(f) computing the pseudoinverse matrix values of said matrix; and

(g) using said pseudoinverse matrix values to determine the electronic currents required to construct said set of desired magnetic field configurations.

13. The method according to claim 12, wherein said method further comprises applying a plurality of coordinately modulated single said electronic shim currents along corresponding ones of a plurality of substantially commonly oriented single said shim paths, said shim paths disposed on a common surface, and suppressing more than one functional component of an inhomogeneity in the magnetic field using the plurality of said electronic shim currents.

14. The method according to claim 12 further comprising the step of

coordinately modulating electronic currents in individual ones of said plurality of shim paths according to said pseudoinverse matrix values.

15. The method according to claim 12, wherein at least a subset of said shim paths are comprised in a shim panel having first and second substantially distanced panel ends and a substantially flat portion, and individual ones of said subset of said shim paths each substantially extend between said panel ends, wherein individual ones of the shim paths have a substantially common overall orientation.

21. A method for constructing a set of desired magnetic field configurations within a magnetic resonance apparatus comprising a plurality of shim paths, the method comprising the steps of:

(a) providing a shim panel having first and second substantially distanced panel ends and a substantially flat portion, said shim panel adapted to comprise at least a subset of said shim paths such that individual ones of said subset of said shim paths each substantially extend between said panel ends, wherein individual ones of the shim paths have a substantially common overall orientation, and wherein said subset of said shim paths are configured for applying electronic shim currents thereon, each of said currents entering a shim path at one said panel end, flowing along said shim path from said one said panel end and exiting said shim path at the other said panel end;

(b) estimating a representation of the magnetic field as a function of spatial coordinate variables produced by a known electronic shim current in a first one of said shim paths by applying said current to said shim path and collecting a spatial map of magnetic field values using a magnetometer probe;

(c) computing a scalar product of (i) a desired magnetic field configuration, and (ii) a magnetic field function estimated according to step (b);

(d) repeating step (b) and step (c) for a plurality of pairs of said desired magnetic field configurations and estimated shimming field functions produced by known electronic shim currents;

(e) arranging the scalar product values of step (d) into a matrix;

(f) computing the pseudoinverse matrix values of said matrix; and

(g) using said pseudoinverse matrix values to determine the electronic currents required to construct said set of desired magnetic field configurations.