Method for controlling the distribution of the RF magnetic field in a magnetic resonance imaging system

Patent metadata

Field	Value
Publication number	US-10816620-B2
Application number	US-201716090460-A
Country	US
Kind code	B2
Filing date	Mar 29, 2017
Priority date	Mar 29, 2016
Publication date	Oct 27, 2020
Grant date	Oct 27, 2020

Abstract

A method for controlling the distribution of the RF magnetic field in a magnetic resonance imaging system, having steps of: placing a cage coil in a permanent magnet supplying a permanent magnetic field along a first axis, and supplying an RF signal to the cage coil in order for the coil to generate an RF magnetic field rotating in a plane that runs perpendicular to the first axis; and putting in place an electromagnetic resonator, the resonance mode of which is excited by the rotating magnetic field, the resonator being placed in a position inside or outside the cage coil and at a distance from a region to be analyzed of an object to be placed in the cage coil, the resonance mode and the position of the resonator in relation to the volumetric antenna being suitable for adjusting the intensity of the rotating magnetic field in an area of the region to be analyzed.

First claim

The invention claimed is:

1. A method of controlling the distribution of a radiofrequency magnetic field in a magnetic resonance imaging system, comprising:
disposing a cage coil in a permanent magnet providing a permanent magnetic field along a first axis;
supplying the cage coil with a single radiofrequency signal so that it generates a radiofrequency magnetic field rotating in a plane perpendicular to the first axis; and
placing an electromagnetic resonator at a position inside or outside the cage coil and at a distance from a region to be analyzed of an object to be arranged in the cage coil, the resonator being electrically connected to nowhere and having a resonance mode excited by the rotating magnetic field, the resonance mode and the position of the resonator relative to the cage coil being adapted to adjust the intensity of the rotating magnetic field in an area of the region to be analyzed.

2. The method of claim 1 , wherein the resonance mode of the resonator is adapted by changing the structure, geometry or size of the resonator, or the nature of the materials forming the resonator.

3. The method of claim 1 , wherein the resonator is configured to have a plurality of resonance modes.

4. The method of claim 1 , wherein the resonator has one of the following configurations:
the resonator is formed by a single rod arranged parallel to the first axis, the rod being rectilinear or folded so as to form meanders, or folded so as to form a rectangular loop, or
the resonator comprises a plurality of parallel conductor rods distributed in a matrix configuration, the rods being embedded in a dielectric material and arranged parallel to the first axis and electromagnetically coupled together.

5. The method of claim 4 , wherein the resonance mode of the resonator is adapted by adjusting the length of the resonator along the first axis or by changing the matrix configuration of the rods.

6. The method of claim 1 , wherein the resonator is disposed in front of a supply port of the cage coil and configured to increase or decrease the rotating magnetic field locally in an area of the region to be analyzed close to the resonator or in an area of the region to be analyzed located opposite the resonator with respect to a center of the region to be analyzed.

7. The method of claim 1 , further comprising:
placing a plurality of electromagnetic resonators, each having a resonance mode excited by the rotating magnetic field, at respective positions inside or outside the cage coil and at said distance from the region to be analyzed, the resonance mode and the position of each of the resonators being adapted to adjust the intensity of the rotating magnetic field in an area of the region to be analyzed.

8. A coil system for a magnetic resonance imaging system, further comprising:
a cage coil configured to receive a single radiofrequency signal for generating inside the cage coil a radiofrequency magnetic field rotating in a plane; and
an electromagnetic resonator electrically connected to nowhere and having a resonance mode excited by the rotating magnetic field, the resonator being placed at a position inside or outside the cage coil and at a distance from a region to be analyzed of an object placed in the cage coil, the resonance mode and the position of the resonator relative to the cage coil being adapted to adjust the intensity of the rotating magnetic field in an area of the region to be analyzed.

9. The coil system of claim 8 , wherein the resonator has one of the following configurations:
the resonator has a periodic structure formed of a juxtaposition of elementary cells, each elementary cell including at least two different materials,
the resonator includes a plurality of parallel conducting rods, distributed in an n×n matrix configuration, n being an integer greater than 0, and embedded in a dielectric material, the resonator being arranged inside or outside the cage coil so that the rods are perpendicular to the plane, or
the resonator is formed by a single rod disposed perpendicular to the plane, the rod being rectilinear or folded so as to form meanders, or folded on itself so as to form an elongated loop extending perpendicular to the plane.

10. The coil system of claim 8 , comprising a plurality of resonators disposed inside or outside the cage coil perpendicular to the plane.

11. The coil system of claim 10 , wherein the resonator comprises 2×2 rods, the rods having a diameter between 0.2 and 1.2 mm, and being spaced apart by 1 to 3 cm, the resonator being located more than 2 cm from the region to be analyzed.

12. The coil system of claim 8 , wherein the resonator is configured to have a resonance mode centered on a frequency of the rotating magnetic field.

13. The coil system of claim 8 , in which the cage coil is a high-pass bird cage comprising 16 bars connecting two rings to each other, each ring segment between two bars of the two rings comprising a capacitor.

14. A magnetic resonance imaging system, comprising:
a cage coil arranged in a permanent magnet providing a permanent magnetic field along a longitudinal axis of the cage coil, the cage coil being configured to receive a single radiofrequency signal for generating inside the cage coil a radiofrequency magnetic field rotating in a plane perpendicular to the longitudinal axis; and perpendicular to the longitudinal axis; and
an electromagnetic resonator electrically connected to nowhere and having a resonance mode excited by the rotating magnetic field, the resonator being placed at a position inside or outside the cage coil and at a distance from a region to be analyzed of an object placed in the cage coil, the resonance mode and the position of the resonator relative to the cage coil being adapted to adjust the intensity of the rotating magnetic field in an area of the region to be analyzed.

15. The system of claim 14 , wherein the permanent magnetic field produced by the permanent magnet is 7 T, the cage coil comprising bars interconnecting two rings, each ring segment of the two rings between two bars comprising a capacitor, the bars having a length between 23 and 27 cm, the rings of the cage coil having a diameter between 24 and 28 cm, and the capacitors having a capacitance between 2 and 6 pF.

16. The system of claim 14 , wherein the resonator has one of the following configurations:
the resonator has a periodic structure formed of a juxtaposition of elementary cells, each elementary cell including at least two different materials,
the resonator includes a plurality of parallel conducting rods, distributed in an n×n matrix configuration, n being an integer greater than 0, and embedded in a dielectric material, the resonator being arranged inside or outside the cage coil so that the rods are perpendicular to the plane, or
the resonator is formed by a single rod disposed perpendicular to the plane, the rod being rectilinear or folded so as to form meanders, or folded on itself so as to form an elongated loop extending perpendicular to the plane.

17. The system of claim 14 , further comprising:
a plurality of resonators disposed inside or outside the cage coil perpendicular to the plane.

18. The system of claim 17 , wherein the resonator comprises 2×2 rods, the rods having a diameter between 0.2 and 1.2 mm, and being spaced apart by 1 to 3 cm, the resonator being located more than 2 cm from the region to be analyzed.

19. The system of claim 14 , wherein the resonator is configured to have a resonance mode centered on a frequency of the rotating magnetic field.

Assignees

• Univ Marseille
• Centre Nat Rech Scient
• Ecole Centrale Marseille
• Commissariat A Grave Over Lenergie Atomique Et Aux Energies Alternatives
• Univ Aix Marseille
• Commissariat Energie Atomique

Inventors

• Abdeddaim Redha
• Enoch Stefan
• Sabouroux Pierre
• Tayeb Gérard Henri Jacques
• Bonod Nicolas
• Vignaud Alexandre Christian
• Larrat Benoit
• Georget Elodie Virginia Emilia
• Leroi Lisa Marie Anna

Classifications

• G01R33/34076 Primary

  Birdcage coils · 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

• G01R33/3642

  Mutual coupling or decoupling of multiple coils, e.g. decoupling of a receive coil from a transmission coil, or intentional coupling of RF coils, e.g. for RF magnetic field amplification · CPC title

• G01R33/34007

  Manufacture of RF coils, e.g. using printed circuit board technology; additional hardware for providing mechanical support to the RF coil assembly or to part thereof, e.g. a support for moving the coil assembly relative to the remainder of the MR system · CPC title

• G01R33/3607

  RF waveform generators, e.g. frequency generators, amplitude-, frequency- or phase modulators or shifters, pulse programmers, digital to analog converters for the RF signal, means for filtering or attenuating of the RF signal · CPC title