Low-inductance transverse litz foil coils

• US 6,060,882 A
• Filed: 06/29/1998
• Issued: 05/09/2000
• Est. Priority Date: 12/29/1995
• Status: Expired due to Term

• Current Assignee: Doty Scientific, Inc.
• Original Assignee: Doty Scientific, Inc.
• Inventors: Doty, F. David
• Primary Examiner(s): Oda, Christine K.
• Assistant Examiner(s): Fetzner, Tiffany A.
• Application Number:
  US09/091,987
• Time in Patent Office: 680 Days
• Field of Search: 324/300-322, 324/318, 600/421
• US Class Current: 324/318
• CPC Class Codes: G01R 33/34007 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 Class Codes: G01R 33/34046 Volume type coils, e.g. bird-cage coils; Quadrature bird-cage coils; Circularly polarised coils
• CPC Class Codes: G01R 33/34092 RF coils specially adapted for NMR spectrometers

Abstract

A family of NMR coils based on Litz foil conductor groups is disclosed. The simplest embodiment is a two-element Litz foil coil. The foils are joined at node (1) and node (2) and are electrically insulated at crossover (3). When the coil is positioned in a plane perpendicular to a uniform magnetic field, the areas (A) defining two flux sub-windows must be equal.

Claims

1. A litz coil formed on the surface of a substantially elliptical coilform for use in a main polarizing magnetic field B_Z for magnetic resonance for the purpose of generating or detecting rf B₁ transverse to the axis of said coilform in, for example, the y-direction inside an external rf shield, said litz coil comprising:

a litz group comprising multiple, parallel, conductor foils having interwoven sub-routes from a first node to a second node and insulated crossovers such that at least two well-defined flux sub-windows are formed,

a first litz semi-coil on the +y side of said coilform comprising at least one litz group and a series-parallel combination of conductors forming axial and azimuthal conductor elements around a central flux window centered on the +y axis,

a second substantially equivalent litz semi-coil on the -y side of said coilform with electrical coupling means to said first litz semi-coil,

said first litz semi-coil further characterized as having leads for connecting to a tuning capacitor,

said sub-routes positioned such that when said litz coil is driven by rf current at a predetermined frequency the total rf magnetic flux through said central flux window is less than 50% of the total rf magnetic flux through the y=0 plane.

2. The litz coil of claim 1 wherein said conductors comprise foil patterns that have been etched on the surfaces of double-clad laminate and said crossovers are connected by feedthroughs between the surfaces of said laminate, said laminate comprising copper cladding over a flexible substrate having low dielectric loss.

3. The litz coil of claim 1 wherein:

said first litz semi-coil comprises 4n litz groups, said litz semi-coil is substantially symmetric with respect to reflections through to two perpendicular planes, and n is a positive integer.

4. The litz coil of claim 1 wherein said flux sub-windows within said litz group have approximately equal areas.

5. The litz coil of claim 1 wherein said flux sub-windows within said litz group are substantially bisected by a plane containing the center of said central flux window and said axis of said coilform.

6. The litz coil of claim 1 wherein said central flux window subtends azimuthal angle less than 85°

.

7. The litz coil of claim 1 wherein the outermost edges of said axial conductor elements subtend azimuthal angle greater than 160°

.

8. The litz coil of claim 1 wherein said substantially elliptical coilform is flexible.

9. The litz coil of claim 1 wherein said elliptical coilform is cylindrical.

10. The litz coil of claim 1 wherein said axis of said coilform is parallel to B_Z.

11. The litz coil of claim 1 wherein said axis of said coilform is inclined at 54.7°

with respect to B_Z.

12. The litz coil of claim 1 wherein the outermost of said azimuthal conductor elements are shielded from the sample by an internal cylindrical rf shield.

13. The litz coil of claim 1 wherein the leads to said tuning capacitor are shielded from the sample.

14. The litz coil of claim 1 wherein said conductor elements execute one turn around said central flux window and a first segmenting capacitor is inserted into a node opposite said tuning capacitor between two series-connected conductor groups of substantially equal inductance, said tuning capacitor and said segmenting capacitor having comparable values.

15. The litz coil of claim 2 wherein said feedthroughs comprise copper foil through slits in said substrate.

16. The litz coil of claim 2 wherein said foil patterns are plated first with a paramagnetic metal and then with a diamagnetic metal such that the magnitude of the total magnetization of the pattern is substantially reduced.

17. The litz coil of claim 2 wherein most of the conductor elements adjacent to said central flux window on the first surface of said laminate are duplicated on the second surface of said laminate and paralleled by suitable feedthroughs.

18. The litz coil of claim 1 further characterized in that the inside edge of a conductor foil has been extended radially outward from said coilform by bending or rolling, where the inside edge is defined as the edge closer to said central flux window.

19. The litz coil of claim 1 wherein said conductor foils have been cut from a multi-layer metallic foil sandwich having magnitude of bulk magnetic susceptibility less than 25% that of pure copper.

20. The litz coil of claim 9 wherein said coilform is made from forsterite.

21. The litz coil of claim 19 wherein said crossovers are insulated with axially aligned, homogeneous, dielectric strips of uniform cross-section and length greater than the sum of the length of said central flux window and the radius of said coilform.

22. The litz coil of claim 2 wherein said litz semi-coil is further characterized as including a litz super-group, said litz super-group comprising a low-inductance litz group in series with a higher inductance conductor group, said litz super-group connected in parallel with a third inductor group.

23. The litz coil of claim 22 wherein said higher inductance conductor group is a litz group.

24. The litz coil of claim 22 wherein said third inductor group is a second litz super-group symmetrically related to said first litz super-group.

25. The litz coil of claim 22 wherein a second segmenting capacitor is inserted between said low-inductance litz group and said higher-inductance conductor group.

26. The litz coil of claim 25 wherein a third segmenting capacitor is inserted into a node in said higher-inductance conductor group.

27. The litz coil of claim 24 wherein the outermost edges of said axial conductor elements subtend azimuthal angle of approximately 174°

, the central flux window subtends azimuthal angle of approximately 56°

, and the diameter of said external rf shield is approximately 1.2 times the mean diameter of said coilform.

28. The litz coil of claim 25 wherein said electrical coupling means comprise tabs near the axial center and at azimuthal location perpendicular to said y axis.

29. The litz coil of claim 1 wherein one of said sub-routes is broken by an audio blocking capacitor, where said audio blocking capacitor has magnitude of reactance X_C that is much less than the reactance X_L of the self inductance of said litz group at the lowest rf frequency of intended use.

30. The litz coil of claim 1 wherein each of said sub-routes is broken by an audio blocking capacitor, where each said blocking capacitor has equal value and each has magnitude of reactance X_C that is less than the reactance X_L of the self inductance of said litz group at the lowest rf frequency of intended use.

31. A litz coil for use in an external polarizing magnetic field B_Z for magnetic resonance for the purpose of generating or detecting rf B₁ transverse to the axis of a sample in, for example, the y-direction, said litz coil comprising:

a litz group comprising multiple, parallel, conductors having interwoven sub-routes from a first node to a second node and insulated crossovers such that at least two well-defined flux sub-windows are formed,

a first litz semi-coil on the +y side of said sample comprising at least one litz group and a series-parallel combination of conductors forming axial and azimuthal conductor elements around a central flux window centered on the +y axis,

a second litz semi-coil on the -y side of said sample with coupling means to said first litz semi-coil,

said first litz semi-coil further characterized as having leads for connecting to a tuning capacitor,

said sub-routes positioned such that when said litz coil is driven by rf current at a predetermined frequency the total rf magnetic flux through said central flux window is less than 80% of the total rf magnetic flux through the y=0 plane.

32. A litz coil for magnetic resonance formed on the surface of a coilform of mean diameter d_C inside an external rf shield of mean diameter sd_C for the purpose of generating or detecting a transverse rf B₁, said coil comprising:

multiple, parallel, interwoven, axial and azimuthal conductor elements circumscribing central flux windows of axial length h₁ on opposite sides of said coilform,

low-inductance leads for connecting said coil to capacitive tuning means,

current paths such that when rf current is applied to said leads at resonance the current in conductor elements adjacent to one of said central flux windows is less than 35% of the sum of the current in all axial elements in one quadrant of said coil and the net flux between adjacent said conductor elements is greater than the 70% of the flux through one of said central flux windows,

effective parallel coil inductance L that satisfies the following over a wide range of frequencies;

##EQU5## where the coefficient has units of nH/mm.

33. A half-turn-fixed-frequency (HTF) rf coil for NMR formed on the surface of an elliptical coilform, said rf coil comprising a first HTF semi-coil on, for example, the +y side of said coilform and a second substantially equivalent HTF semi-coil on the -y side of said coilform with electrical coupling means to said first HTF semi-coil, said first HTF semi-coil comprising,

a segmented outer saddle loop executing one turn around said +y axis, said outer loop subtending mean azimuthal angle greater than 125°

but less than 155°

,

segmenting capacitors at opposite axial ends of said outer loop,

an unsegmented inner loop executing one turn around a central flux window centered on said +y axis and subtending azimuthal angle greater than 50°

but less than 80°

, said inner loop connected in parallel with one of said segmenting capacitors.

34. A quadrature litz coil approximately aligned with the main polarizing magnetic field B_Z for magnetic resonance for the purpose of generating or detecting a rotating transverse rf B₁ inside an external cylindrical rf shield, said quadrature litz coil comprising two concentric litz coils of slightly differing diameters rotated 90°

with respect to the other, each said litz coil tuned to resonate at the same frequency and each comprising;

a litz group comprising multiple, parallel, conductors having interwoven sub-routes from a first node to a second node and insulated crossovers such that at least two well-defined litz flux sub-windows are formed,

a first litz semi-coil on, for example, the +y side of said coilform comprising at least one litz group and a series-parallel combination of conductors forming axial and azimuthal conductor elements around a central flux window centered on the +y axis,

a second substantially equivalent litz semi-coil on the -y side of said coilform with electrical coupling means to said first litz semi-coil,

said first litz semi-coil further characterized as having leads for connecting to a tuning capacitor,

said sub-routes positioned such that when said litz coil is driven by rf current at a predetermined frequency the total rf magnetic flux through said central flux window is less than 50% of the total rf magnetic flux through the y=0 plane.

35. A quadrature litz birdcage coil approximately aligned with the main polarizing magnetic field B_Z for magnetic resonance for the purpose of generating or detecting a rotating transverse rf B₁ inside an external cylindrical rf shield, said quadrature litz birdcage coil comprising a conventional MRI birdcage coil in which a plurality of conductor elements have been replaced by litz groups, where a litz group comprises multiple, parallel, conductor foils having interwoven sub-routes from a first node to a second node and insulated crossovers such that at least two well-defined flux sub-windows are formed.

36. A quadrature litz birdcage coil approximately aligned with the main polarizing magnetic field B_Z for magnetic resonance for the purpose of generating or detecting a rotating transverse rf B₁ inside an external cylindrical rf shield, said quadrature litz birdcage coil comprising a conventional MRI birdcage coil in which a plurality of conductor elements have been replaced with conventional litz wire.

37. The quadrature litz birdcage coil of 36 wherein said litz wire is loosely woven and spread out to cover a greater portion of the surface area of said coil.